Merge branch 'dev' into em/dev

This commit is contained in:
Lindsey Heagy
2016-05-09 11:32:59 -07:00
29 changed files with 1912 additions and 596 deletions
+4
View File
@@ -25,6 +25,10 @@ SimPEG
:target: https://coveralls.io/r/simpeg/simpeg?branch=master
:alt: Coverage status
.. image:: http://img.shields.io/badge/GITTER-JOIN_CHAT-brightgreen.svg?style=flat-square
:alt: gitter chat room at https://gitter.im/simpeg/simpeg
:target: https://gitter.im/simpeg/simpeg
Simulation and Parameter Estimation in Geophysics - A python package for simulation and gradient based parameter estimation in the context of geophysical applications.
The vision is to create a package for finite volume simulation with applications to geophysical imaging and subsurface flow. To enable the understanding of the many different components, this package has the following features:
+244 -96
View File
@@ -169,7 +169,7 @@ def readUBC_DC2DModel(fileName):
return model
def plot_pseudoSection(DCsurvey, axs, stype):
def plot_pseudoSection(DCsurvey, axs, stype='dpdp', dtype="appc", clim=None, cblabel=True, axlabel = True, colorbar = True, contour = None):
"""
Read list of 2D tx-rx location and plot a speudo-section of apparent
resistivity.
@@ -179,7 +179,7 @@ def plot_pseudoSection(DCsurvey, axs, stype):
Input:
:param d2D, z0
:switch stype -> Either 'pdp' (pole-dipole) | 'dpdp' (dipole-dipole)
:switch dtype=-> Either 'appr' (app. res) | 'appc' (app. con) | 'volt' (potential)
Output:
:figure scatter plot overlayed on image
@@ -192,9 +192,6 @@ def plot_pseudoSection(DCsurvey, axs, stype):
from scipy.interpolate import griddata
import pylab as plt
# Set depth to 0 for now
z0 = 0.
# Pre-allocate
midx = []
midz = []
@@ -221,47 +218,97 @@ def plot_pseudoSection(DCsurvey, axs, stype):
Cmid = (Tx[0][0] + Tx[1][0])/2
Pmid = (Rx[0][:,0] + Rx[1][:,0])/2
# Compute pant leg of apparent rho
if stype == 'pdp':
leg = data * 2*np.pi * MA * ( MA + MN ) / MN
# Change output for dtype
if dtype == 'volt':
leg = np.log10(abs(1/leg))
rho = np.hstack([rho,data])
elif stype == 'dpdp':
leg = data * 2*np.pi / ( 1/MA - 1/MB - 1/NB + 1/NA )
else:
# Compute pant leg of apparent rho
if stype == 'pdp':
leg = data * 2*np.pi * MA * ( MA + MN ) / MN
elif stype == 'dpdp':
leg = data * 2*np.pi / ( 1/MA - 1/MB - 1/NB + 1/NA )
else:
print """dtype must be 'pdp'(pole-dipole) | 'dpdp' (dipole-dipole) """
break
if dtype == 'appc':
leg = np.log10(abs(1./leg))
rho = np.hstack([rho,leg])
elif dtype == 'appr':
leg = np.log10(abs(leg))
rho = np.hstack([rho,leg])
else:
print """dtype must be 'appr' | 'appc' | 'volt' """
break
midx = np.hstack([midx, ( Cmid + Pmid )/2 ])
midz = np.hstack([midz, -np.abs(Cmid-Pmid)/2 + z0 ])
rho = np.hstack([rho,leg])
ax = axs
midz = np.hstack([midz, -np.abs(Cmid-Pmid)/2 + (Tx[0][2] + Tx[1][2])/2 ])
# Grid points
grid_x, grid_z = np.mgrid[np.min(midx):np.max(midx), np.min(midz):np.max(midz)]
grid_rho = griddata(np.c_[midx,midz], rho.T, (grid_x, grid_z), method='linear')
# Scale the color scheme
if clim == None:
vmin, vmax = rho.min(), rho.max()
else:
vmin, vmax = clim[0], clim[1]
# Plot data
grid_rho = np.ma.masked_where(np.isnan(grid_rho), grid_rho)
ph = plt.pcolormesh(grid_x[:,0],grid_z[0,:],grid_rho.T, vmin = vmin, vmax = vmax)
plt.gca().tick_params(axis='both', which='major', labelsize=8)
if contour is not None:
plt.contour(grid_x,grid_z,grid_rho,levels = contour,colors = 'r', vmin = vmin, vmax = vmax)
# Add scatter points
axs.scatter(midx,midz,s=10,c=rho.T, vmin = vmin, vmax = vmax)
if colorbar:
if dtype == 'volt':
cbar = plt.colorbar(ph, ax = axs, format="%4.1f",fraction=0.04,orientation="horizontal")
else:
cbar = plt.colorbar(ph, ax = axs, format="$10^{%.1f}$",fraction=0.04,orientation="horizontal")
cmin,cmax = cbar.get_clim()
ticks = np.linspace(cmin,cmax,3)
cbar.set_ticks(ticks)
cbar.ax.tick_params(labelsize=10)
if cblabel:
if dtype == 'appc':
cbar.set_label("App.Cond",size=12)
elif dtype == 'appr':
cbar.set_label("App.Res.",size=12)
elif dtype == 'volt':
cbar.set_label("Potential (V)",size=12)
plt.imshow(grid_rho.T, extent = (np.min(midx),np.max(midx),np.min(midz),np.max(midz)), origin='lower', alpha=0.8, vmin = np.min(rho), vmax = np.max(rho))
cbar = plt.colorbar(format = '%.2f',fraction=0.04,orientation="horizontal")
cmin,cmax = cbar.get_clim()
ticks = np.linspace(cmin,cmax,3)
cbar.set_ticks(ticks)
if not axlabel:
axs.set_xticklabels([])
axs.set_yticklabels([])
# Plot apparent resistivity
plt.scatter(midx,midz,s=50,c=rho.T)
ax.set_xticklabels([])
ax.set_ylabel('Z')
ax.yaxis.tick_right()
ax.yaxis.set_label_position('right')
plt.gca().set_aspect('equal', adjustable='box')
return ax
return ph
def gen_DCIPsurvey(endl, mesh, stype, a, b, n):
"""
@@ -361,16 +408,6 @@ def gen_DCIPsurvey(endl, mesh, stype, a, b, n):
srcClass = DC.SrcDipole([rxClass], M[ii,:],M[ii,:])
SrcList.append(srcClass)
#==============================================================================
# elif re.match(stype,'dpdp'):
#
# for ii in range(0, int(nstn)-2):
#
# indx = np.min([ii+n+1,nstn])
# Tx.append(np.c_[M[ii,:],N[ii,:]])
# Rx.append(np.c_[M[ii+2:indx,:],N[ii+2:indx,:]])
#==============================================================================
elif stype == 'gradient':
# Gradient survey only requires Tx at end of line and creates a square
@@ -423,15 +460,15 @@ def gen_DCIPsurvey(endl, mesh, stype, a, b, n):
survey = DC.SurveyDC(SrcList)
return survey, Tx, Rx
def writeUBC_DCobs(fileName, DCsurvey, dtype, stype):
def writeUBC_DCobs(fileName, DCsurvey, dtype='3D', stype='SURFACE', iptype = 0):
"""
Write UBC GIF DCIP 2D or 3D observation file
Input:
:string fileName -> including path where the file is written out
:DCsurvey -> DC survey class object
:string dtype -> either '2D' | '3D'
:string stype -> either 'SURFACE' | 'GENERAL'
:string fileName -> including path where the file is written out
:DCsurvey DC survey class object
:string dtype -> either '2D' | '3D'
:string stype -> either 'SURFACE' | 'GENERAL'
Output:
:param UBC2D-Data file
@@ -446,10 +483,16 @@ def writeUBC_DCobs(fileName, DCsurvey, dtype, stype):
assert (dtype=='2D') | (dtype=='3D'), "Data must be either '2D' | '3D'"
assert (stype=='SURFACE') | (stype=='GENERAL') | (stype=='SIMPLE'), "Data must be either 'SURFACE' | 'GENERAL' | 'SIMPLE'"
fid = open(fileName,'w')
fid.write('! ' + stype + ' FORMAT\n')
if iptype!=0:
fid.write('IPTYPE=%i\n'%iptype)
else:
fid.write('! ' + stype + ' FORMAT\n')
count = 0
for ii in range(DCsurvey.nSrc):
@@ -473,7 +516,7 @@ def writeUBC_DCobs(fileName, DCsurvey, dtype, stype):
B = np.repeat(tx[0,1],M.shape[0],axis=0)
M = M[:,0]
N = N[:,0]
np.savetxt(fid, np.c_[A, B, M, N , DCsurvey.dobs[count:count+nD], DCsurvey.std[count:count+nD] ], fmt='%e',delimiter=' ',newline='\n')
@@ -481,18 +524,25 @@ def writeUBC_DCobs(fileName, DCsurvey, dtype, stype):
if stype == 'SURFACE':
fid.writelines("%e " % ii for ii in mkvc(tx[0,:]))
fid.writelines("%f " % ii for ii in mkvc(tx[0,:]))
M = M[:,0]
N = N[:,0]
if stype == 'GENERAL':
# Flip sign for z-elevation to depth
tx[2::2,:] = -tx[2::2,:]
fid.writelines("%e " % ii for ii in mkvc(tx[::2,:]))
M = M[:,0::2]
N = N[:,0::2]
# Flip sign for z-elevation to depth
M[:,1::2] = -M[:,1::2]
N[:,1::2] = -N[:,1::2]
fid.write('%i\n'% nD)
np.savetxt(fid, np.c_[ M, N , DCsurvey.dobs[count:count+nD], DCsurvey.std[count:count+nD] ], fmt='%e',delimiter=' ',newline='\n')
np.savetxt(fid, np.c_[ M, N , DCsurvey.dobs[count:count+nD], DCsurvey.std[count:count+nD] ], fmt='%f',delimiter=' ',newline='\n')
if dtype=='3D':
@@ -504,31 +554,32 @@ def writeUBC_DCobs(fileName, DCsurvey, dtype, stype):
if stype == 'GENERAL':
fid.writelines("%e " % ii for ii in mkvc(tx))
fid.writelines("%e " % ii for ii in mkvc(tx[0:3,:]))
fid.write('%i\n'% nD)
np.savetxt(fid, np.c_[ M, N , DCsurvey.dobs[count:count+nD], DCsurvey.std[count:count+nD] ], fmt='%e',delimiter=' ',newline='\n')
fid.write('\n')
count += nD
fid.close()
def convertObs_DC3D_to_2D(DCsurvey,lineID):
def convertObs_DC3D_to_2D(DCsurvey,lineID, flag = 'local'):
"""
Read DC survey and data and change
coordinate system to distance along line assuming
all data is acquired along line.
First transmitter pole is assumed to be at the origin
Read DC survey and projects the coordinate system
according to the flag = 'Xloc' | 'Yloc' | 'local' (default)
In the 'local' system, station coordinates are referenced
to distance from the first srcLoc[0].loc[0]
Assumes flat topo for now...
The Z value is preserved, but Y coordinates zeroed.
Input:
:param Tx, Rx
:param survey3D
Output:
:figure Tx2d, Rx2d
:figure survey2D
Edited Feb 17th, 2016
Edited April 6th, 2016
@author: dominiquef
@@ -570,25 +621,39 @@ def convertObs_DC3D_to_2D(DCsurvey,lineID):
Rx = DCsurvey.srcList[indx[ii]].rxList[0].locs
nrx = Rx[0].shape[0]
# Find A electrode along line
vec, r = r_unit(x0,Tx[ii][0,0:2])
A = stn_id(vecTx,vec,r)
if flag == 'local':
# Find A electrode along line
vec, r = r_unit(x0,Tx[ii][0,0:2])
A = stn_id(vecTx,vec,r)
# Find B electrode along line
vec, r = r_unit(x0,Tx[ii][1,0:2])
B = stn_id(vecTx,vec,r)
# Find B electrode along line
vec, r = r_unit(x0,Tx[ii][1,0:2])
B = stn_id(vecTx,vec,r)
M = np.zeros(nrx)
N = np.zeros(nrx)
for kk in range(nrx):
M = np.zeros(nrx)
N = np.zeros(nrx)
for kk in range(nrx):
# Find all M electrodes along line
vec, r = r_unit(x0,Rx[0][kk,0:2])
M[kk] = stn_id(vecTx,vec,r)
# Find all M electrodes along line
vec, r = r_unit(x0,Rx[0][kk,0:2])
M[kk] = stn_id(vecTx,vec,r)
# Find all N electrodes along line
vec, r = r_unit(x0,Rx[1][kk,0:2])
N[kk] = stn_id(vecTx,vec,r)
# Find all N electrodes along line
vec, r = r_unit(x0,Rx[1][kk,0:2])
N[kk] = stn_id(vecTx,vec,r)
elif flag == 'Yloc':
""" Flip the XY axis locs"""
A = Tx[ii][0,1]
B = Tx[ii][1,1]
M = Rx[0][:,1]
N = Rx[1][:,1]
elif flag == 'Xloc':
""" Copy the rx-tx locs"""
A = Tx[ii][0,0]
B = Tx[ii][1,0]
M = Rx[0][:,0]
N = Rx[1][:,0]
Rx = DC.RxDipole(np.c_[M,np.zeros(nrx),Rx[0][:,2]],np.c_[N,np.zeros(nrx),Rx[1][:,2]])
@@ -601,51 +666,59 @@ def convertObs_DC3D_to_2D(DCsurvey,lineID):
DCsurvey2D.std = np.asarray(DCsurvey.std)
return DCsurvey2D
def readUBC_DC3Dobs(fileName):
def readUBC_DC3Dobs(fileName, dtype = 'DC'):
"""
Read UBC GIF DCIP 3D observation file and generate arrays for tx-rx location
Read UBC GIF IP 3D observation file and generate survey
Input:
:param fileName, path to the UBC GIF 3D obs file
Output:
:param rx, tx, d, wd
:param IPsurvey
:return
Created on Mon December 7th, 2015
@author: dominiquef
"""
zflag = True # Flag for z value provided
# Load file
obsfile = np.genfromtxt(fileName,delimiter=' \n',dtype=np.str,comments='!')
if dtype == 'IP':
obsfile = np.genfromtxt(fileName,delimiter=' \n',dtype=np.str,comments='IPTYPE')
elif dtype == 'DC':
obsfile = np.genfromtxt(fileName,delimiter=' \n',dtype=np.str,comments='!')
else:
print "dtype must be 'DC'(default) | 'IP'"
# Pre-allocate
srcLists = []
Rx = []
d = []
wd = []
zflag = True # Flag for z value provided
# Countdown for number of obs/tx
count = 0
for ii in range(obsfile.shape[0]):
# Skip if blank line
if not obsfile[ii]:
continue
# First line is transmitter with number of receivers
# First line or end of a transmitter block, read transmitter info
if count==0:
temp = (np.fromstring(obsfile[ii], dtype=float,sep=' ').T)
# Read the line
temp = (np.fromstring(obsfile[ii], dtype=float, sep=' ').T)
count = int(temp[-1])
# Check if z value is provided, if False -> nan
if len(temp)==5:
tx = np.r_[temp[0:2],np.nan,temp[0:2],np.nan]
zflag = False
tx = np.r_[temp[0:2],np.nan,temp[2:4],np.nan]
zflag = False # Pass on the flag to the receiver loc
else:
tx = temp[:-1]
@@ -653,8 +726,16 @@ def readUBC_DC3Dobs(fileName):
rx = []
continue
temp = np.fromstring(obsfile[ii], dtype=float,sep=' ')
temp = np.fromstring(obsfile[ii], dtype=float,sep=' ') # Get the string
# Filter out negative IP
# if temp[-2] < 0:
# count = count -1
# print "Negative!"
#
# else:
# If the Z-location is provided, otherwise put nan
if zflag:
rx.append(temp[:-2])
@@ -664,7 +745,7 @@ def readUBC_DC3Dobs(fileName):
wd.append(temp[-1])
else:
rx.append(np.r_[temp[0:2],np.nan,temp[0:2],np.nan] )
rx.append(np.r_[temp[0:2],np.nan,temp[2:4],np.nan] )
# Check if there is data with the location
if len(temp)==6:
d.append(temp[-2])
@@ -672,7 +753,7 @@ def readUBC_DC3Dobs(fileName):
count = count -1
# Reach the end of transmitter block
# Reach the end of transmitter block, append the src, rx and continue
if count == 0:
rx = np.asarray(rx)
Rx = DC.RxDipole(rx[:,:3],rx[:,3:])
@@ -688,6 +769,7 @@ def readUBC_DC3Dobs(fileName):
def readUBC_DC2Dobs(fileName):
"""
------- NEEDS TO BE UPDATED ------
Read UBC GIF 2D observation file and generate arrays for tx-rx location
Input:
@@ -735,6 +817,73 @@ def readUBC_DC2Dobs(fileName):
return tx, rx, d, wd
def readUBC_DC2Dpre(fileName):
"""
Read UBC GIF DCIP 2D observation file and generate arrays for tx-rx location
Input:
:param fileName, path to the UBC GIF 3D obs file
Output:
DCsurvey
:return
Created on Mon March 9th, 2016 << Doug's 70th Birthday !! >>
@author: dominiquef
"""
# Load file
obsfile = np.genfromtxt(fileName,delimiter=' \n',dtype=np.str,comments='!')
# Pre-allocate
srcLists = []
Rx = []
d = []
zflag = True # Flag for z value provided
for ii in range(obsfile.shape[0]):
if not obsfile[ii]:
continue
# First line is transmitter with number of receivers
temp = (np.fromstring(obsfile[ii], dtype=float,sep=' ').T)
# Check if z value is provided, if False -> nan
if len(temp)==5:
tx = np.r_[temp[0],np.nan,np.nan,temp[1],np.nan,np.nan]
zflag = False
else:
tx = np.r_[temp[0],np.nan,temp[1],temp[2],np.nan,temp[3]]
if zflag:
rx = np.c_[temp[4],np.nan,temp[5],temp[6],np.nan,temp[7]]
else:
rx = np.c_[temp[2],np.nan,np.nan,temp[3],np.nan,np.nan]
# Check if there is data with the location
d.append(temp[-1])
Rx = DC.RxDipole(rx[:,:3],rx[:,3:])
srcLists.append( DC.SrcDipole( [Rx], tx[:3],tx[3:]) )
# Create survey class
survey = DC.SurveyDC(srcLists)
survey.dobs = np.asarray(d)
return {'DCsurvey':survey}
def readUBC_DC2DMesh(fileName):
"""
Read UBC GIF 2DTensor mesh and generate 2D Tensor mesh in simpeg
@@ -928,7 +1077,6 @@ def getSrc_locs(DCsurvey):
srcMat = np.zeros((DCsurvey.nSrc,2,3))
for ii in range(DCsurvey.nSrc):
print np.asarray(DCsurvey.srcList[ii].loc).shape
srcMat[ii,:,:] = np.asarray(DCsurvey.srcList[ii].loc)
return srcMat
+124 -36
View File
@@ -216,13 +216,13 @@ class SaveOutputDictEveryIteration(_SaveEveryIteration):
# Save the data.
ms = self.reg.Ws * ( self.reg.mapping * (self.invProb.curModel - self.reg.mref) )
phi_ms = 0.5*ms.dot(ms)
if self.reg.smoothModel == True:
if self.reg.mrefInSmooth == True:
mref = self.reg.mref
else:
mref = 0
mx = self.reg.Wx * ( self.reg.mapping * (self.invProb.curModel - mref) )
phi_mx = 0.5 * mx.dot(mx)
if self.prob.mesh.dim==2:
if self.prob.mesh.dim >= 2:
my = self.reg.Wy * ( self.reg.mapping * (self.invProb.curModel - mref) )
phi_my = 0.5 * my.dot(my)
else:
@@ -237,40 +237,6 @@ class SaveOutputDictEveryIteration(_SaveEveryIteration):
# Save the file as a npz
np.savez('{:03d}-{:s}'.format(self.opt.iter,self.fileName), iter=self.opt.iter, beta=self.invProb.beta, phi_d=self.invProb.phi_d, phi_m=self.invProb.phi_m, phi_ms=phi_ms, phi_mx=phi_mx, phi_my=phi_my, phi_mz=phi_mz,f=self.opt.f, m=self.invProb.curModel,dpred=self.invProb.dpred)
class SaveOutputDictEveryIteration(_SaveEveryIteration):
"""SaveOutputDictEveryIteration
A directive that saves some relevant information from the inversion run to a numpy .npz dictionary file (see numpy.savez function for further info).
"""
def initialize(self):
print "SimPEG.SaveOutputDictEveryIteration will save your inversion progress as dictionary: '%s-###.npz'"%self.fileName
def endIter(self):
# Save the data.
ms = self.reg.Ws * ( self.reg.mapping * (self.invProb.curModel - self.reg.mref) )
phi_ms = 0.5*ms.dot(ms)
if self.reg.smoothModel == True:
mref = self.reg.mref
else:
mref = 0
mx = self.reg.Wx * ( self.reg.mapping * (self.invProb.curModel - mref) )
phi_mx = 0.5 * mx.dot(mx)
if self.prob.mesh.dim==2:
my = self.reg.Wy * ( self.reg.mapping * (self.invProb.curModel - mref) )
phi_my = 0.5 * my.dot(my)
else:
phi_my = 'NaN'
if self.prob.mesh.dim==3 and 'CYL' not in self.prob.mesh._meshType:
mz = self.reg.Wz * ( self.reg.mapping * (self.invProb.curModel - mref) )
phi_mz = 0.5 * mz.dot(mz)
else:
phi_mz = 'NaN'
# Save the file as a npz
np.savez('{:s}-{:03d}'.format(self.fileName,self.opt.iter), iter=self.opt.iter, beta=self.invProb.beta, phi_d=self.invProb.phi_d, phi_m=self.invProb.phi_m, phi_ms=phi_ms, phi_mx=phi_mx, phi_my=phi_my, phi_mz=phi_mz,f=self.opt.f, m=self.invProb.curModel,dpred=self.invProb.dpred)
# class UpdateReferenceModel(Parameter):
@@ -283,3 +249,125 @@ class SaveOutputDictEveryIteration(_SaveEveryIteration):
# mref = self.mref0
# self.m_prev = self.invProb.m_current
# return mref
class Update_IRLS(InversionDirective):
eps_min = None
factor = None
gamma = None
phi_m_last = None
phi_d_last = None
def initialize(self):
# Scale the regularization for changes in norm
if getattr(self, 'phi_m_last', None) is not None:
self.reg.curModel = self.invProb.curModel
self.reg.gamma = 1.
phim_new = self.reg.eval(self.invProb.curModel)
self.gamma = self.phi_m_last / phim_new
self.reg.curModel = self.invProb.curModel
self.reg.gamma = self.gamma
if getattr(self, 'phi_d_last', None) is None:
self.phi_d_last = self.invProb.phi_d
def endIter(self):
# Cool the threshold parameter if required
if getattr(self, 'factor', None) is not None:
eps = self.reg.eps / self.factor
if getattr(self, 'eps_min', None) is not None:
self.reg.eps = np.max([self.eps_min,eps])
else:
self.reg.eps = eps
# Get phi_m at the end of current iteration
self.phi_m_last = self.invProb.phi_m_last
# Update the model used for the IRLS weights
self.reg.curModel = self.invProb.curModel
# Temporarely set gamma to 1. to get raw phi_m
self.reg.gamma = 1.
# Compute new model objective function value
phim_new = self.reg.eval(self.invProb.curModel)
# Update gamma to scale the regularization between IRLS iterations
self.reg.gamma = self.phi_m_last / phim_new
# Set the weighting matrix to None so that it is recomputed next time
# it is called in the inversion
self.reg._W = None
class Update_lin_PreCond(InversionDirective):
"""
Create a Jacobi preconditioner for the linear problem
"""
onlyOnStart=False
def initialize(self):
if getattr(self.opt, 'approxHinv', None) is None:
# Update the pre-conditioner
diagA = np.sum(self.prob.G**2.,axis=0) + self.invProb.beta*(self.reg.W.T*self.reg.W).diagonal() #* (self.reg.mapping * np.ones(self.reg.curModel.size))**2.
PC = Utils.sdiag((self.prob.mapping.deriv(None).T *diagA)**-1.)
self.opt.approxHinv = PC
def endIter(self):
# Cool the threshold parameter
if self.onlyOnStart==True:
return
if getattr(self.opt, 'approxHinv', None) is not None:
# Update the pre-conditioner
diagA = np.sum(self.prob.G**2.,axis=0) + self.invProb.beta*(self.reg.W.T*self.reg.W).diagonal() #* (self.reg.mapping * np.ones(self.reg.curModel.size))**2.
PC = Utils.sdiag((self.prob.mapping.deriv(None).T *diagA)**-1.)
self.opt.approxHinv = PC
class Update_Wj(InversionDirective):
"""
Create approx-sensitivity base weighting using the probing method
"""
k = None # Number of probing cycles
itr = None # Iteration number to update Wj, or always update if None
def endIter(self):
if self.itr is None or self.itr == self.opt.iter:
m = self.invProb.curModel
if self.k is None:
self.k = int(self.survey.nD/10)
def JtJv(v):
Jv = self.prob.Jvec(m, v)
return self.prob.Jtvec(m,Jv)
JtJdiag = Utils.diagEst(JtJv,len(m),k=self.k)
JtJdiag = JtJdiag / max(JtJdiag)
self.reg.wght = JtJdiag
class Scale_Beta(InversionDirective):
"""
Instead of a linear cooling schedule, beta is allowed to change based
on the ratio between the target misfit and the current data misfit. The
update is done only if the misfit is outside some threshold bounds.
"""
tol = 0.05
def endIter(self):
# Check if misfit is within the tolerance, otherwise adjust beta
val = self.invProb.phi_d / (self.survey.nD*0.5)
if np.abs(1.-val) > self.tol:
self.invProb.beta = self.invProb.beta * self.survey.nD*0.5 / self.invProb.phi_d
+48 -25
View File
@@ -2,19 +2,27 @@ from SimPEG import Mesh, Utils, np, sp
import SimPEG.DCIP as DC
import time
def run(loc=None, sig=None, radi=None, param=None, stype='dpdp', plotIt=True):
def run(loc=None, sig=None, radi=None, param=None, stype='dpdp', dtype='appc', plotIt=True):
"""
DC Forward Simulation
=====================
Forward model conductive spheres in a half-space and plot a pseudo-section
Forward model two conductive spheres in a half-space and plot a
pseudo-section. Assumes an infinite line source and measures along the
center of the spheres.
Created by @fourndo on Mon Feb 01 19:28:06 2016
INPUT:
loc = Location of spheres [[x1,y1,z1],[x2,y2,z2]]
radi = Radius of spheres [r1,r2]
param = Conductivity of background and two spheres [m0,m1,m2]
stype = survey type "pdp" (pole dipole) or "dpdp" (dipole dipole)
dtype = Data type "appr" (app res) | "appc" (app cond) | "volt" (potential)
Created by @fourndo
"""
assert stype in ['pdp', 'dpdp'], "Source type (stype) must be pdp or dpdp (pole dipole or dipole dipole)"
assert dtype in ['appr', 'appc', 'volt'], "Data type (dtype) must be appr (app res) or appc (app cond) or volt (potential)"
if loc is None:
loc = np.c_[[-50.,0.,-50.],[50.,0.,-50.]]
@@ -27,7 +35,6 @@ def run(loc=None, sig=None, radi=None, param=None, stype='dpdp', plotIt=True):
# First we need to create a mesh and a model.
# This is our mesh
dx = 5.
@@ -52,14 +59,10 @@ def run(loc=None, sig=None, radi=None, param=None, stype='dpdp', plotIt=True):
# Get index of the center
indy = int(mesh.nCy/2)
# Plot the model for reference
# Define core mesh extent
xlim = 200
zlim = 125
# Specify the survey type: "pdp" | "dpdp"
zlim = 100
# Then specify the end points of the survey. Let's keep it simple for now and survey above the anomalies, top of the mesh
ends = [(-175,0),(175,0)]
@@ -77,12 +80,13 @@ def run(loc=None, sig=None, radi=None, param=None, stype='dpdp', plotIt=True):
dl_len = np.sqrt( np.sum((locs[0,:] - locs[1,:])**2) )
dl_x = ( Tx[-1][0,1] - Tx[0][0,0] ) / dl_len
dl_y = ( Tx[-1][1,1] - Tx[0][1,0] ) / dl_len
azm = np.arctan(dl_y/dl_x)
#azm = np.arctan(dl_y/dl_x)
#Set boundary conditions
mesh.setCellGradBC('neumann')
# Define the differential operators needed for the DC problem
# Define the linear system needed for the DC problem. We assume an infitite
# line source for simplicity.
Div = mesh.faceDiv
Grad = mesh.cellGrad
Msig = Utils.sdiag(1./(mesh.aveF2CC.T*(1./model)))
@@ -145,16 +149,23 @@ def run(loc=None, sig=None, radi=None, param=None, stype='dpdp', plotIt=True):
print 'Forward completed'
# Let's just convert the 3D format into 2D (distance along line) and plot
# [Tx2d, Rx2d] = DC.convertObs_DC3D_to_2D(survey, np.ones(survey.nSrc))
survey2D = DC.convertObs_DC3D_to_2D(survey, np.ones(survey.nSrc))
survey2D = DC.convertObs_DC3D_to_2D(survey, np.ones(survey.nSrc) , 'Xloc')
survey2D.dobs =np.hstack(data)
# Here is an example for the first tx-rx array
if plotIt:
import matplotlib.pyplot as plt
fig = plt.figure()
fig = plt.figure(figsize=(7,7))
ax = plt.subplot(2,1,1, aspect='equal')
mesh.plotSlice(np.log10(model), ax =ax, normal = 'Y', ind = indy,grid=True)
ax.set_title('E-W section at '+str(mesh.vectorCCy[indy])+' m')
# Plot the location of the spheres for reference
circle1=plt.Circle((loc[0,0],loc[2,0]),radi[0],color='w',fill=False, lw=3)
circle2=plt.Circle((loc[0,1],loc[2,1]),radi[1],color='k',fill=False, lw=3)
ax.add_artist(circle1)
ax.add_artist(circle2)
dat = mesh.plotSlice(np.log10(model), ax =ax, normal = 'Y',
ind = indy,grid=True, clim = np.log10([sig.min(),sig.max()]))
ax.set_title('3-D model')
plt.gca().set_aspect('equal', adjustable='box')
plt.scatter(Tx[0][0,:],Tx[0][2,:],s=40,c='g', marker='v')
@@ -163,22 +174,34 @@ def run(loc=None, sig=None, radi=None, param=None, stype='dpdp', plotIt=True):
plt.ylim([-zlim,mesh.vectorNz[-1]+dx])
ax = plt.subplot(2,1,2, aspect='equal')
pos = ax.get_position()
ax.set_position([pos.x0 , pos.y0 + 0.025 , pos.width, pos.height])
pos = ax.get_position()
cbarax = fig.add_axes([pos.x0 , pos.y0 + 0.025 , pos.width, pos.height * 0.04]) ## the parameters are the specified position you set
cb = fig.colorbar(dat[0],cax=cbarax, orientation="horizontal",
ax = ax, ticks=np.linspace(np.log10(sig.min()),
np.log10(sig.max()), 3), format="$10^{%.1f}$")
cb.set_label("Conductivity (S/m)",size=12)
cb.ax.tick_params(labelsize=12)
# Second plot for the predicted apparent resistivity data
ax2 = plt.subplot(2,1,2, aspect='equal')
# Plot the location of the spheres for reference
circle1=plt.Circle((loc[0,0]-Tx[0][0,0],loc[2,0]),radi[0],color='w',fill=False, lw=3)
circle2=plt.Circle((loc[0,1]-Tx[0][0,0],loc[2,1]),radi[1],color='k',fill=False, lw=3)
ax.add_artist(circle1)
ax.add_artist(circle2)
circle1=plt.Circle((loc[0,0],loc[2,0]),radi[0],color='w',fill=False, lw=3)
circle2=plt.Circle((loc[0,1],loc[2,1]),radi[1],color='k',fill=False, lw=3)
ax2.add_artist(circle1)
ax2.add_artist(circle2)
# Add the speudo section
DC.plot_pseudoSection(survey2D,ax,stype)
dat = DC.plot_pseudoSection(survey2D,ax2,stype=stype, dtype = dtype)
# plt.scatter(Tx2d[0][:],Tx[0][2,:],s=40,c='g', marker='v')
# plt.scatter(Rx2d[0][:],Rx[0][:,2::3],s=40,c='y')
# plt.plot(np.r_[Tx2d[0][0],Rx2d[-1][-1,-1]],np.ones(2)*mesh.vectorNz[-1], color='k')
plt.ylim([-zlim,mesh.vectorNz[-1]+dx])
ax2.set_title('Apparent Conductivity data')
plt.ylim([-zlim,mesh.vectorNz[-1]+dx])
plt.show()
return fig, ax
+1 -2
View File
@@ -48,8 +48,7 @@ def run(plotIt=True):
freqs = np.logspace(1,3,10)
srcLoc = np.array([0., 0., 10.])
srcList = []
[srcList.append(EM.FDEM.Src.MagDipole([bzi],freq, srcLoc,orientation='Z')) for freq in freqs]
srcList = [EM.FDEM.Src.MagDipole([bzi],freq, srcLoc,orientation='Z') for freq in freqs]
survey = EM.FDEM.Survey(srcList)
prb = EM.FDEM.Problem3D_b(mesh, mapping=mapping)
@@ -0,0 +1,275 @@
from SimPEG import *
from SimPEG.EM import FDEM, Analytics, mu_0
import time
try:
from pymatsolver import MumpsSolver
solver = MumpsSolver
except Exception:
solver = SolverLU
pass
def run(plotIt=True):
"""
EM: Schenkel and Morrison Casing Model
======================================
Here we create and run a FDEM forward simulation to calculate the vertical
current inside a steel-cased. The model is based on the Schenkel and
Morrison Casing Model, and the results are used in a 2016 SEG abstract by
Yang et al.
- Schenkel, C.J., and H.F. Morrison, 1990, Effects of well casing on potential field measurements using downhole current sources: Geophysical prospecting, 38, 663-686.
The model consists of:
- Air: Conductivity 1e-8 S/m, above z = 0
- Background: conductivity 1e-2 S/m, below z = 0
- Casing: conductivity 1e6 S/m
- 300m long
- radius of 0.1m
- thickness of 6e-3m
Inside the casing, we take the same conductivity as the background.
We are using an EM code to simulate DC, so we use frequency low enough
that the skin depth inside the casing is longer than the casing length (f
= 1e-6 Hz). The plot produced is of the current inside the casing.
These results are shown in the SEG abstract by Yang et al., 2016: 3D DC
resistivity modeling of steel casing for reservoir monitoring using
equivalent resistor network. The solver used to produce these results and
achieve the CPU time of ~30s is Mumps, which was installed using pymatsolver_
.. _pymatsolver: https://github.com/rowanc1/pymatsolver
This example is on figshare: https://dx.doi.org/10.6084/m9.figshare.3126961.v1
If you would use this example for a code comparison, or build upon it, a
citation would be much appreciated!
"""
if plotIt:
import matplotlib.pylab as plt
# ------------------ MODEL ------------------
sigmaair = 1e-8 # air
sigmaback = 1e-2 # background
sigmacasing = 1e6 # casing
sigmainside = sigmaback # inside the casing
casing_t = 0.006 # 1cm thickness
casing_l = 300 # length of the casing
casing_r = 0.1
casing_a = casing_r - casing_t/2. # inner radius
casing_b = casing_r + casing_t/2. # outer radius
casing_z = np.r_[-casing_l,0.]
# ------------------ SURVEY PARAMETERS ------------------
freqs = np.r_[1e-6] #[1e-1, 1, 5] # frequencies
dsz = -300 # down-hole z source location
src_loc = np.r_[0.,0.,dsz]
inf_loc = np.r_[0.,0.,1e4]
print 'Skin Depth: ', [(500./np.sqrt(sigmaback*_)) for _ in freqs]
# ------------------ MESH ------------------
# fine cells near well bore
csx1, csx2 = 2e-3, 60.
pfx1, pfx2 = 1.3, 1.3
ncx1 = np.ceil(casing_b/csx1+2)
# pad nicely to second cell size
npadx1 = np.floor(np.log(csx2/csx1) / np.log(pfx1))
hx1a,hx1b = Utils.meshTensor([(csx1,ncx1)]),Utils.meshTensor([(csx1,npadx1,pfx1)])
dx1 = sum(hx1a)+sum(hx1b)
dx1 = np.floor(dx1/csx2)
hx1b *= (dx1*csx2 - sum(hx1a))/sum(hx1b)
# second chunk of mesh
dx2 = 300. # uniform mesh out to here
ncx2 = np.ceil((dx2 - dx1)/csx2)
npadx2 = 45
hx2a, hx2b = Utils.meshTensor([(csx2,ncx2)]), Utils.meshTensor([(csx2,npadx2,pfx2)])
hx = np.hstack([hx1a,hx1b,hx2a,hx2b])
# z-direction
csz = 0.05
nza = 10
ncz, npadzu, npadzd = np.int(np.ceil(np.diff(casing_z)[0]/csz))+10, 68, 68 # cell size, number of core cells, number of padding cells in the x- direction
hz = Utils.meshTensor([(csz,npadzd,-1.3), (csz,ncz), (csz,npadzu,1.3)]) # vector of cell widths in the z-direction
# Mesh
mesh = Mesh.CylMesh([hx,1.,hz], [0.,0.,-np.sum(hz[:npadzu+ncz-nza])])
print 'Mesh Extent xmax: %f,: zmin: %f, zmax: %f'%(mesh.vectorCCx.max(), mesh.vectorCCz.min(), mesh.vectorCCz.max())
print 'Number of cells', mesh.nC
if plotIt is True:
fig, ax = plt.subplots(1, 1, figsize=(6, 4))
ax.set_title('Simulation Mesh')
mesh.plotGrid(ax=ax)
plt.show()
# Put the model on the mesh
sigWholespace = sigmaback*np.ones((mesh.nC))
sigBack = sigWholespace.copy()
sigBack[mesh.gridCC[:,2] > 0.] = sigmaair
sigCasing = sigBack.copy()
iCasingZ = (mesh.gridCC[:,2] <= casing_z[1]) & (mesh.gridCC[:,2] >= casing_z[0])
iCasingX = (mesh.gridCC[:,0] >= casing_a) & (mesh.gridCC[:,0] <= casing_b)
iCasing = iCasingX & iCasingZ
sigCasing[iCasing] = sigmacasing
if plotIt is True:
# plotting parameters
xlim = np.r_[0., 0.2]
zlim = np.r_[-350., 10.]
clim_sig = np.r_[-8,6]
# plot models
fig, ax = plt.subplots(1,1,figsize=(4,4))
f = plt.colorbar(mesh.plotImage(np.log10(sigCasing),ax=ax)[0], ax=ax)
ax.grid(which='both')
ax.set_title('Log_10 (Sigma)')
ax.set_xlim(xlim)
ax.set_ylim(zlim)
f.set_clim(clim_sig)
plt.show()
# -------------- Sources --------------------
# Define Custom Current Sources
# surface source
sg_x = np.zeros(mesh.vnF[0],dtype=complex)
sg_y = np.zeros(mesh.vnF[1],dtype=complex)
sg_z = np.zeros(mesh.vnF[2],dtype=complex)
nza = 2 # put the wire two cells above the surface
ncin = 2
# vertically directed wire
sgv_indx = (mesh.gridFz[:,0] > casing_a) & (mesh.gridFz[:,0] < casing_a + csx1) # hook it up to casing at the surface
sgv_indz = (mesh.gridFz[:,2] <= +csz*nza) & (mesh.gridFz[:,2] >= -csz*2)
sgv_ind = sgv_indx & sgv_indz
sg_z[sgv_ind] = -1.
# horizontally directed wire
sgh_indx = (mesh.gridFx[:,0] > casing_a) & (mesh.gridFx[:,0] <= inf_loc[2])
sgh_indz = (mesh.gridFx[:,2] > csz*(nza-0.5)) & (mesh.gridFx[:,2] < csz*(nza+0.5))
sgh_ind = sgh_indx & sgh_indz
sg_x[sgh_ind] = -1.
sgv2_indx = (mesh.gridFz[:,0] >= mesh.gridFx[sgh_ind,0].max()) & (mesh.gridFz[:,0] <= inf_loc[2]*1.2) # hook it up to casing at the surface
sgv2_indz = (mesh.gridFz[:,2] <= +csz*nza) & (mesh.gridFz[:,2] >= -csz*2)
sgv2_ind = sgv2_indx & sgv2_indz
sg_z[sgv2_ind] = 1.
# assemble the source
sg = np.hstack([sg_x,sg_y,sg_z])
sg_p = [FDEM.Src.RawVec_e([],_,sg/mesh.area) for _ in freqs]
# downhole source
dg_x = np.zeros(mesh.vnF[0],dtype=complex)
dg_y = np.zeros(mesh.vnF[1],dtype=complex)
dg_z = np.zeros(mesh.vnF[2],dtype=complex)
# vertically directed wire
dgv_indx = (mesh.gridFz[:,0] < csx1) # go through the center of the well
dgv_indz = (mesh.gridFz[:,2] <= +csz*nza) & (mesh.gridFz[:,2] > dsz + csz/2.)
dgv_ind = dgv_indx & dgv_indz
dg_z[dgv_ind] = -1.
# couple to the casing downhole
dgh_indx = mesh.gridFx[:,0] < casing_a + csx1
dgh_indz = (mesh.gridFx[:,2] < dsz + csz) & (mesh.gridFx[:,2] >= dsz)
dgh_ind = dgh_indx & dgh_indz
dg_x[dgh_ind] = 1.
# horizontal part at surface
dgh2_indx = mesh.gridFx[:,0] <= inf_loc[2]*1.2
dgh2_indz = sgh_indz.copy()
dgh2_ind = dgh2_indx & dgh2_indz
dg_x[dgh2_ind] = -1.
# vertical part at surface
dgv2_ind = sgv2_ind.copy()
dg_z[dgv2_ind] = 1.
# assemble the source
dg = np.hstack([dg_x,dg_y,dg_z])
dg_p = [FDEM.Src.RawVec_e([],_,dg/mesh.area) for _ in freqs]
# ------------ Problem and Survey ---------------
survey = FDEM.Survey(sg_p + dg_p)
mapping = [('sigma', Maps.IdentityMap(mesh))]
problem = FDEM.Problem_h(mesh, mapping=mapping)
problem.pair(survey)
# ------------- Solve ---------------------------
t0 = time.time()
fieldsCasing = problem.fields(sigCasing)
print 'Time to solve 2 sources', time.time() - t0
# Plot current
# current density
jn0 = fieldsCasing[dg_p,'j']
jn1 = fieldsCasing[sg_p,'j']
# current
in0 = [mesh.area*fieldsCasing[dg_p,'j'][:,i] for i in range(len(freqs))]
in1 = [mesh.area*fieldsCasing[sg_p,'j'][:,i] for i in range(len(freqs))]
in0 = np.vstack(in0).T
in1 = np.vstack(in1).T
# integrate to get z-current inside casing
inds_inx = (mesh.gridFz[:,0] >= casing_a) & (mesh.gridFz[:,0] <= casing_b)
inds_inz = (mesh.gridFz[:,2] >= dsz ) & (mesh.gridFz[:,2] <= 0)
inds_fz = inds_inx & inds_inz
indsx = [False]*mesh.nFx
inds = list(indsx) + list(inds_fz)
in0_in = in0[np.r_[inds]]
in1_in = in1[np.r_[inds]]
z_in = mesh.gridFz[inds_fz,2]
in0_in = in0_in.reshape([in0_in.shape[0]/3,3])
in1_in = in1_in.reshape([in1_in.shape[0]/3,3])
z_in = z_in.reshape([z_in.shape[0]/3,3])
I0 = in0_in.sum(1).real
I1 = in1_in.sum(1).real
z_in = z_in[:,0]
if plotIt is True:
fig, ax = plt.subplots(1,2,figsize=(12,4))
ax[0].plot(z_in,np.absolute(I0), z_in,np.absolute(I1))
ax[0].legend(['top casing', 'bottom casing'],loc='best')
ax[0].set_title('Magnitude of Vertical Current in Casing')
ax[1].semilogy(z_in,np.absolute(I0), z_in,np.absolute(I1))
ax[1].legend(['top casing', 'bottom casing'],loc='best')
ax[1].set_title('Magnitude of Vertical Current in Casing')
ax[1].set_ylim([1e-2, 1.])
plt.show()
if __name__ == '__main__':
run()
+132
View File
@@ -0,0 +1,132 @@
from SimPEG import *
def run(N=200, plotIt=True):
"""
Inversion: Linear Problem
=========================
Here we go over the basics of creating a linear problem and inversion.
"""
np.random.seed(1)
std_noise = 1e-2
mesh = Mesh.TensorMesh([N])
m0 = np.ones(mesh.nC) * 1e-4
nk = 10
jk = np.linspace(1.,nk,nk)
p = -2.
q = 1.
g = lambda k: np.exp(p*jk[k]*mesh.vectorCCx)*np.cos(np.pi*q*jk[k]*mesh.vectorCCx)
G = np.empty((nk, mesh.nC))
for i in range(nk):
G[i,:] = g(i)
mtrue = np.zeros(mesh.nC)
mtrue[mesh.vectorCCx > 0.3] = 1.
mtrue[mesh.vectorCCx > 0.45] = -0.5
mtrue[mesh.vectorCCx > 0.6] = 0
prob = Problem.LinearProblem(mesh, G)
survey = Survey.LinearSurvey()
survey.pair(prob)
survey.dobs = prob.fields(mtrue) + std_noise * np.random.randn(nk)
#survey.makeSyntheticData(mtrue, std=std_noise)
wd = np.ones(nk) * std_noise
#print survey.std[0]
#M = prob.mesh
# Distance weighting
wr = np.sum(prob.G**2.,axis=0)**0.5
wr = ( wr/np.max(wr) )
reg = Regularization.Simple(mesh)
reg.wght = wr
dmis = DataMisfit.l2_DataMisfit(survey)
dmis.Wd = 1./wd
opt = Optimization.ProjectedGNCG(maxIter=30,lower=-2.,upper=2., maxIterCG= 20, tolCG = 1e-4)
invProb = InvProblem.BaseInvProblem(dmis, reg, opt)
invProb.curModel = m0
beta = Directives.BetaSchedule(coolingFactor=2, coolingRate=1)
target = Directives.TargetMisfit()
betaest = Directives.BetaEstimate_ByEig()
inv = Inversion.BaseInversion(invProb, directiveList=[beta, betaest, target])
mrec = inv.run(m0)
ml2 = mrec
print "Final misfit:" + str(invProb.dmisfit.eval(mrec))
# Switch regularization to sparse
phim = invProb.phi_m_last
phid = invProb.phi_d
reg = Regularization.Sparse(mesh)
#==============================================================================
# fig, axes = plt.subplots(1,2,figsize=(12*1.2,4*1.2))
# dmdx = reg.mesh.cellDiffxStencil * mrec
# plt.plot(np.sort(dmdx))
#==============================================================================
#reg.recModel = mrec
reg.wght = np.ones(mesh.nC)
reg.mref = np.zeros(mesh.nC)
reg.eps_p = 5e-2
reg.eps_q = 1e-2
reg.norms = [0., 0., 2., 2.]
reg.wght = wr
opt = Optimization.ProjectedGNCG(maxIter=10 ,lower=-2.,upper=2., maxIterLS = 20, maxIterCG= 20, tolCG = 1e-3)
invProb = InvProblem.BaseInvProblem(dmis, reg, opt, beta = invProb.beta*2.)
beta = Directives.BetaSchedule(coolingFactor=1, coolingRate=1)
#betaest = Directives.BetaEstimate_ByEig()
target = Directives.TargetMisfit()
IRLS =Directives.Update_IRLS( phi_m_last = phim, phi_d_last = phid )
inv = Inversion.BaseInversion(invProb, directiveList=[beta,IRLS])
m0 = mrec
# Run inversion
mrec = inv.run(m0)
print "Final misfit:" + str(invProb.dmisfit.eval(mrec))
if plotIt:
import matplotlib.pyplot as plt
fig, axes = plt.subplots(1,2,figsize=(12*1.2,4*1.2))
for i in range(prob.G.shape[0]):
axes[0].plot(prob.G[i,:])
axes[0].set_title('Columns of matrix G')
axes[1].plot(mesh.vectorCCx, mtrue, 'b-')
axes[1].plot(mesh.vectorCCx, ml2, 'r-')
#axes[1].legend(('True Model', 'Recovered Model'))
axes[1].set_ylim(-1.0,1.25)
axes[1].plot(mesh.vectorCCx, mrec, 'k-',lw = 2)
axes[1].legend(('True Model', 'Smooth l2-l2',
'Sparse lp:' + str(reg.norms[0]) + ', lqx:' + str(reg.norms[1]) ), fontsize = 12)
plt.show()
return prob, survey, mesh, mrec
if __name__ == '__main__':
run()
+1 -1
View File
@@ -100,7 +100,7 @@ def run(plotIt=True):
# Regularization - with a regularization mesh
regMesh = simpeg.Mesh.TensorMesh([m1d.hx[problem.mapping.sigmaMap.maps[-1].indActive]],m1d.x0)
reg = simpeg.Regularization.Tikhonov(regMesh)
reg.smoothModel = True
reg.mrefInSmooth = True
reg.alpha_s = 1e-7
reg.alpha_x = 1.
# Inversion problem
+3 -1
View File
@@ -5,9 +5,11 @@ import DC_Analytic_Dipole
import DC_Forward_PseudoSection
import EM_FDEM_1D_Inversion
import EM_FDEM_Analytic_MagDipoleWholespace
import EM_Schenkel_Morrison_Casing
import EM_TDEM_1D_Inversion
import FLOW_Richards_1D_Celia1990
import Forward_BasicDirectCurrent
import Inversion_IRLS
import Inversion_Linear
import Mesh_Basic_PlotImage
import Mesh_Basic_Types
@@ -19,7 +21,7 @@ import Mesh_Tensor_Creation
import MT_1D_ForwardAndInversion
import MT_3D_Foward
__examples__ = ["DC_Analytic_Dipole", "DC_Forward_PseudoSection", "EM_FDEM_1D_Inversion", "EM_FDEM_Analytic_MagDipoleWholespace", "EM_TDEM_1D_Inversion", "FLOW_Richards_1D_Celia1990", "Forward_BasicDirectCurrent", "Inversion_Linear", "Mesh_Basic_PlotImage", "Mesh_Basic_Types", "Mesh_Operators_CahnHilliard", "Mesh_QuadTree_Creation", "Mesh_QuadTree_FaceDiv", "Mesh_QuadTree_HangingNodes", "Mesh_Tensor_Creation", "MT_1D_ForwardAndInversion", "MT_3D_Foward"]
__examples__ = ["DC_Analytic_Dipole", "DC_Forward_PseudoSection", "EM_FDEM_1D_Inversion", "EM_FDEM_Analytic_MagDipoleWholespace", "EM_Schenkel_Morrison_Casing", "EM_TDEM_1D_Inversion", "FLOW_Richards_1D_Celia1990", "Forward_BasicDirectCurrent", "Inversion_IRLS", "Inversion_Linear", "Mesh_Basic_PlotImage", "Mesh_Basic_Types", "Mesh_Operators_CahnHilliard", "Mesh_QuadTree_Creation", "Mesh_QuadTree_FaceDiv", "Mesh_QuadTree_HangingNodes", "Mesh_Tensor_Creation", "MT_1D_ForwardAndInversion", "MT_3D_Foward"]
##### AUTOIMPORTS #####
+3 -1
View File
@@ -33,7 +33,9 @@ class BaseInversion(object):
self._directiveList = value
self._directiveList.inversion = self
def __init__(self, invProb, directiveList=[], **kwargs):
def __init__(self, invProb, directiveList=None, **kwargs):
if directiveList is None:
directiveList = []
self.directiveList = directiveList
Utils.setKwargs(self, **kwargs)
+12 -7
View File
@@ -7,17 +7,16 @@ from SimPEG.MT.Utils.dataUtils import rec2ndarr
# Import modules
import numpy as np
import os, sys, re
try:
import osr
except ImportError as e:
print 'Could not import osr, missing the gdal package'
pass
class EDIimporter:
"""
A class to import EDIfiles.
"""
# Define data converters
_impUnitEDI2SI = 4*np.pi*1e-4 # Convert Z[mV/km/nT] (as in EDI)to Z[V/A] SI unit
_impUnitSI2EDI = 1./_impUnitEDI2SI # ConvertZ[V/A] SI unit to Z[mV/km/nT] (as in EDI)
@@ -26,8 +25,8 @@ class EDIimporter:
comps = None
# Hidden properties
_outEPSG = None
_2out = None
_outEPSG = None # Project info
_2out = None # The projection operator
def __init__(self, EDIfilesList, compList=None, outEPSG=None):
@@ -113,6 +112,12 @@ class EDIimporter:
# nOutData=length(obj.data);
# obj.data(nOutData+1:nOutData+length(TEMP.data),:) = TEMP.data;
def _transfromPoints(self,longD,latD):
# Import the coordinate projections
try:
import osr
except ImportError as e:
print 'Could not import osr, missing the gdal package\nCan not project coordinates'
raise e
# Coordinates convertor
if self._2out is None:
src = osr.SpatialReference()
+26 -11
View File
@@ -759,15 +759,29 @@ class PolyMap(IdentityMap):
m = [\sigma_1, \sigma_2, c]
Can take in an actInd vector to account for topography.
"""
def __init__(self, mesh, order, logSigma=True, normal='X'):
def __init__(self, mesh, order, logSigma=True, normal='X', actInd = None):
IdentityMap.__init__(self, mesh)
self.logSigma = logSigma
self.order = order
self.normal = normal
self.actInd = actInd
if getattr(self, 'actInd', None) is None:
self.actInd = range(self.mesh.nC)
self.nC = self.mesh.nC
else:
self.nC = len(self.actInd)
slope = 1e4
@property
def shape(self):
return (self.nC, self.nP)
@property
def nP(self):
if np.isscalar(self.order):
@@ -785,8 +799,8 @@ class PolyMap(IdentityMap):
sig1, sig2 = np.exp(sig1), np.exp(sig2)
#2D
if self.mesh.dim == 2:
X = self.mesh.gridCC[:,0]
Y = self.mesh.gridCC[:,1]
X = self.mesh.gridCC[self.actInd,0]
Y = self.mesh.gridCC[self.actInd,1]
if self.normal =='X':
f = polynomial.polyval(Y, c) - X
elif self.normal =='Y':
@@ -795,9 +809,9 @@ class PolyMap(IdentityMap):
raise(Exception("Input for normal = X or Y or Z"))
#3D
elif self.mesh.dim == 3:
X = self.mesh.gridCC[:,0]
Y = self.mesh.gridCC[:,1]
Z = self.mesh.gridCC[:,2]
X = self.mesh.gridCC[self.actInd,0]
Y = self.mesh.gridCC[self.actInd,1]
Z = self.mesh.gridCC[self.actInd,2]
if self.normal =='X':
f = polynomial.polyval2d(Y, Z, c.reshape((self.order[0]+1,self.order[1]+1))) - X
elif self.normal =='Y':
@@ -806,6 +820,7 @@ class PolyMap(IdentityMap):
f = polynomial.polyval2d(X, Y, c.reshape((self.order[0]+1,self.order[1]+1))) - Z
else:
raise(Exception("Input for normal = X or Y or Z"))
else:
raise(Exception("Only supports 2D"))
@@ -819,8 +834,8 @@ class PolyMap(IdentityMap):
sig1, sig2 = np.exp(sig1), np.exp(sig2)
#2D
if self.mesh.dim == 2:
X = self.mesh.gridCC[:,0]
Y = self.mesh.gridCC[:,1]
X = self.mesh.gridCC[self.actInd,0]
Y = self.mesh.gridCC[self.actInd,1]
if self.normal =='X':
f = polynomial.polyval(Y, c) - X
@@ -832,9 +847,9 @@ class PolyMap(IdentityMap):
raise(Exception("Input for normal = X or Y or Z"))
#3D
elif self.mesh.dim == 3:
X = self.mesh.gridCC[:,0]
Y = self.mesh.gridCC[:,1]
Z = self.mesh.gridCC[:,2]
X = self.mesh.gridCC[self.actInd,0]
Y = self.mesh.gridCC[self.actInd,1]
Z = self.mesh.gridCC[self.actInd,2]
if self.normal =='X':
f = polynomial.polyval2d(Y, Z, c.reshape((self.order[0]+1,self.order[1]+1))) - X
+12 -9
View File
@@ -330,7 +330,7 @@ class CylMesh(BaseTensorMesh, BaseRectangularMesh, InnerProducts, CylView):
raise NotImplementedError('wrapping in the averaging is not yet implemented')
return self._aveF2CCV
def getInterpolationMatCartMesh(self, Mrect, locType='CC'):
def getInterpolationMatCartMesh(self, Mrect, locType='CC', locTypeTo=None):
"""
Takes a cartesian mesh and returns a projection to translate onto the cartesian grid.
"""
@@ -338,19 +338,22 @@ class CylMesh(BaseTensorMesh, BaseRectangularMesh, InnerProducts, CylView):
assert self.isSymmetric, "Currently we have not taken into account other projections for more complicated CylMeshes"
if locTypeTo is None:
locTypeTo = locType
if locType == 'F':
# do this three times for each component
X = self.getInterpolationMatCartMesh(Mrect, locType='Fx')
Y = self.getInterpolationMatCartMesh(Mrect, locType='Fy')
Z = self.getInterpolationMatCartMesh(Mrect, locType='Fz')
X = self.getInterpolationMatCartMesh(Mrect, locType='Fx', locTypeTo=locTypeTo+'x')
Y = self.getInterpolationMatCartMesh(Mrect, locType='Fy', locTypeTo=locTypeTo+'y')
Z = self.getInterpolationMatCartMesh(Mrect, locType='Fz', locTypeTo=locTypeTo+'z')
return sp.vstack((X,Y,Z))
if locType == 'E':
X = self.getInterpolationMatCartMesh(Mrect, locType='Ex')
Y = self.getInterpolationMatCartMesh(Mrect, locType='Ey')
Z = spzeros(Mrect.nEz, self.nE)
X = self.getInterpolationMatCartMesh(Mrect, locType='Ex', locTypeTo=locTypeTo+'x')
Y = self.getInterpolationMatCartMesh(Mrect, locType='Ey', locTypeTo=locTypeTo+'y')
Z = spzeros(getattr(Mrect, 'n' + locTypeTo + 'z'), self.nE)
return sp.vstack((X,Y,Z))
grid = getattr(Mrect, 'grid' + locType)
grid = getattr(Mrect, 'grid' + locTypeTo)
# This is unit circle stuff, 0 to 2*pi, starting at x-axis, rotating counter clockwise in an x-y slice
theta = - np.arctan2(grid[:,0] - self.cartesianOrigin[0], grid[:,1] - self.cartesianOrigin[1]) + np.pi/2
theta[theta < 0] += np.pi*2.0
@@ -366,7 +369,7 @@ class CylMesh(BaseTensorMesh, BaseRectangularMesh, InnerProducts, CylView):
'Ex': Mrect.tangents[:Mrect.nEx,:],
'Ey': Mrect.tangents[Mrect.nEx:(Mrect.nEx+Mrect.nEy),:],
'Ez': Mrect.tangents[-Mrect.nEz:,:],
}[locType]
}[locTypeTo]
if 'F' in locType:
normals = np.c_[np.cos(theta), np.sin(theta), np.zeros(theta.size)]
proj = ( normals * dotMe ).sum(axis=1)
+49 -30
View File
@@ -307,24 +307,28 @@ class DiffOperators(object):
return BC
_cellGradBC_list = 'neumann'
def _cellGradStencil(self):
BC = self.setCellGradBC(self._cellGradBC_list)
n = self.vnC
if(self.dim == 1):
G = ddxCellGrad(n[0], BC[0])
elif(self.dim == 2):
G1 = sp.kron(speye(n[1]), ddxCellGrad(n[0], BC[0]))
G2 = sp.kron(ddxCellGrad(n[1], BC[1]), speye(n[0]))
G = sp.vstack((G1, G2), format="csr")
elif(self.dim == 3):
G1 = kron3(speye(n[2]), speye(n[1]), ddxCellGrad(n[0], BC[0]))
G2 = kron3(speye(n[2]), ddxCellGrad(n[1], BC[1]), speye(n[0]))
G3 = kron3(ddxCellGrad(n[2], BC[2]), speye(n[1]), speye(n[0]))
G = sp.vstack((G1, G2, G3), format="csr")
return G
def cellGrad():
doc = "The cell centered Gradient, takes you to cell faces."
def fget(self):
if(self._cellGrad is None):
BC = self.setCellGradBC(self._cellGradBC_list)
n = self.vnC
if(self.dim == 1):
G = ddxCellGrad(n[0], BC[0])
elif(self.dim == 2):
G1 = sp.kron(speye(n[1]), ddxCellGrad(n[0], BC[0]))
G2 = sp.kron(ddxCellGrad(n[1], BC[1]), speye(n[0]))
G = sp.vstack((G1, G2), format="csr")
elif(self.dim == 3):
G1 = kron3(speye(n[2]), speye(n[1]), ddxCellGrad(n[0], BC[0]))
G2 = kron3(speye(n[2]), ddxCellGrad(n[1], BC[1]), speye(n[0]))
G3 = kron3(ddxCellGrad(n[2], BC[2]), speye(n[1]), speye(n[0]))
G = sp.vstack((G1, G2, G3), format="csr")
G = self._cellGradStencil()
# Compute areas of cell faces & volumes
S = self.area
V = self.aveCC2F*self.vol # Average volume between adjacent cells
@@ -361,19 +365,24 @@ class DiffOperators(object):
_cellGradBC = None
cellGradBC = property(**cellGradBC())
def _cellGradxStencil(self):
BC = ['neumann', 'neumann']
n = self.vnC
if(self.dim == 1):
G1 = ddxCellGrad(n[0], BC)
elif(self.dim == 2):
G1 = sp.kron(speye(n[1]), ddxCellGrad(n[0], BC))
elif(self.dim == 3):
G1 = kron3(speye(n[2]), speye(n[1]), ddxCellGrad(n[0], BC))
return G1
def cellGradx():
doc = "Cell centered Gradient in the x dimension. Has neumann boundary conditions."
def fget(self):
if getattr(self, '_cellGradx', None) is None:
BC = ['neumann', 'neumann']
n = self.vnC
if(self.dim == 1):
G1 = ddxCellGrad(n[0], BC)
elif(self.dim == 2):
G1 = sp.kron(speye(n[1]), ddxCellGrad(n[0], BC))
elif(self.dim == 3):
G1 = kron3(speye(n[2]), speye(n[1]), ddxCellGrad(n[0], BC))
G1 = self._cellGradxStencil()
# Compute areas of cell faces & volumes
V = self.aveCC2F*self.vol
L = self.r(self.area/V, 'F','Fx', 'V')
@@ -382,17 +391,22 @@ class DiffOperators(object):
return locals()
cellGradx = property(**cellGradx())
def _cellGradyStencil(self):
if self.dim < 2: return None
BC = ['neumann', 'neumann']
n = self.vnC
if(self.dim == 2):
G2 = sp.kron(ddxCellGrad(n[1], BC), speye(n[0]))
elif(self.dim == 3):
G2 = kron3(speye(n[2]), ddxCellGrad(n[1], BC), speye(n[0]))
return G2
def cellGrady():
doc = "Cell centered Gradient in the x dimension. Has neumann boundary conditions."
def fget(self):
if self.dim < 2: return None
if getattr(self, '_cellGrady', None) is None:
BC = ['neumann', 'neumann']
n = self.vnC
if(self.dim == 2):
G2 = sp.kron(ddxCellGrad(n[1], BC), speye(n[0]))
elif(self.dim == 3):
G2 = kron3(speye(n[2]), ddxCellGrad(n[1], BC), speye(n[0]))
G2 = self._cellGradyStencil()
# Compute areas of cell faces & volumes
V = self.aveCC2F*self.vol
L = self.r(self.area/V, 'F','Fy', 'V')
@@ -401,14 +415,19 @@ class DiffOperators(object):
return locals()
cellGrady = property(**cellGrady())
def _cellGradzStencil(self):
if self.dim < 3: return None
BC = ['neumann', 'neumann']
n = self.vnC
G3 = kron3(ddxCellGrad(n[2], BC), speye(n[1]), speye(n[0]))
return G3
def cellGradz():
doc = "Cell centered Gradient in the x dimension. Has neumann boundary conditions."
def fget(self):
if self.dim < 3: return None
if getattr(self, '_cellGradz', None) is None:
BC = ['neumann', 'neumann']
n = self.vnC
G3 = kron3(ddxCellGrad(n[2], BC), speye(n[1]), speye(n[0]))
G3 = self._cellGradzStencil()
# Compute areas of cell faces & volumes
V = self.aveCC2F*self.vol
L = self.r(self.area/V, 'F','Fz', 'V')
+1 -2
View File
@@ -21,10 +21,9 @@ class TensorMeshIO(object):
if '*' in seg:
st = seg
sp = seg.split('*')
re = np.array(sp[0],dtype=int)*(' ' + sp[1])
re = int(sp[0])*(' ' + sp[1])
line = line.replace(st,re.strip())
return np.array(line.split(),dtype=float)
# Read the file as line strings, remove lines with comment = !
msh = np.genfromtxt(fileName,delimiter='\n',dtype=np.str,comments='!')
+9 -3
View File
@@ -2131,10 +2131,16 @@ class TreeMesh(BaseTensorMesh, InnerProducts, TreeMeshIO):
def plotSlice(self, v, vType='CC',
normal='Z', ind=None, grid=True, view='real',
ax=None, clim=None, showIt=False,
pcolorOpts={},
streamOpts={'color':'k'},
gridOpts={'color':'k', 'alpha':0.5}):
pcolorOpts=None,
streamOpts=None,
gridOpts=None):
if pcolorOpts is None:
pcolorOpts = {}
if streamOpts is None:
streamOpts = {'color':'k'}
if gridOpts is None:
gridOpts = {'color':'k', 'alpha':0.5}
assert vType in ['CC','F','E']
assert self.dim == 3
+27 -9
View File
@@ -42,9 +42,9 @@ class TensorView(object):
def plotImage(self, v, vType='CC', grid=False, view='real',
ax=None, clim=None, showIt=False,
pcolorOpts={},
streamOpts={'color':'k'},
gridOpts={'color':'k'},
pcolorOpts=None,
streamOpts=None,
gridOpts=None,
numbering=True, annotationColor='w'
):
"""
@@ -84,6 +84,12 @@ class TensorView(object):
M.plotImage(v, annotationColor='k', showIt=True)
"""
if pcolorOpts is None:
pcolorOpts = {}
if streamOpts is None:
streamOpts = {'color':'k'}
if gridOpts is None:
gridOpts = {'color':'k'}
if ax is None:
fig = plt.figure()
@@ -174,9 +180,9 @@ class TensorView(object):
def plotSlice(self, v, vType='CC',
normal='Z', ind=None, grid=False, view='real',
ax=None, clim=None, showIt=False,
pcolorOpts={},
streamOpts={'color':'k'},
gridOpts={'color':'k', 'alpha':0.5}
pcolorOpts=None,
streamOpts=None,
gridOpts=None
):
"""
@@ -197,6 +203,12 @@ class TensorView(object):
M.plotSlice(M.cellGrad*b, 'F', view='vec', grid=True, showIt=True, pcolorOpts={'alpha':0.8})
"""
if pcolorOpts is None:
pcolorOpts = {}
if streamOpts is None:
streamOpts = {'color':'k'}
if gridOpts is None:
gridOpts = {'color':'k', 'alpha':0.5}
if type(vType) in [list, tuple]:
assert ax is None, "cannot specify an axis to plot on with this function."
fig, axs = plt.subplots(1,len(vType))
@@ -289,11 +301,17 @@ class TensorView(object):
def _plotImage2D(self, v, vType='CC', grid=False, view='real',
ax=None, clim=None, showIt=False,
pcolorOpts={},
streamOpts={'color':'k'},
gridOpts={'color':'k'}
pcolorOpts=None,
streamOpts=None,
gridOpts=None
):
if pcolorOpts is None:
pcolorOpts = {}
if streamOpts is None:
streamOpts = {'color':'k'}
if gridOpts is None:
gridOpts = {'color':'k'}
vTypeOptsCC = ['N','CC','Fx','Fy','Ex','Ey']
vTypeOptsV = ['CCv','F','E']
vTypeOpts = vTypeOptsCC + vTypeOptsV
+18
View File
@@ -888,6 +888,8 @@ class ProjectedGNCG(BFGS, Minimize, Remember):
maxIterCG = 5
tolCG = 1e-1
stepOffBoundsFact = 0.1 # perturbation of the inactive set off the bounds
lower = -np.inf
upper = np.inf
@@ -990,4 +992,20 @@ class ProjectedGNCG(BFGS, Minimize, Remember):
cgFlag = 1
# End CG Iterations
# Take a gradient step on the active cells if exist
if temp != self.xc.size:
rhs_a = (Active) * -self.g
dm_i = max( abs( delx ) )
dm_a = max( abs(rhs_a) )
# perturb inactive set off of bounds so that they are included in the step
delx = delx + self.stepOffBoundsFact * (rhs_a * dm_i / dm_a)
# Only keep gradients going in the right direction on the active set
indx = ((self.xc<=self.lower) & (delx < 0)) | ((self.xc>=self.upper) & (delx > 0))
delx[indx] = 0.
return delx
+520 -300
View File
@@ -1,5 +1,289 @@
import Utils, Maps, Mesh, numpy as np, scipy.sparse as sp
class RegularizationMesh(object):
"""
**Regularization Mesh**
This contains the operators used in the regularization. Note that these
are not necessarily true differential operators, but are constructed from
a SimPEG Mesh.
:param Mesh mesh: problem mesh
:param numpy.array indActive: bool array, size nC, that is True where we have active cells. Used to reduce the operators so we regularize only on active cells
"""
def __init__(self, mesh, indActive=None):
self.mesh = mesh
assert indActive is None or indActive.dtype == 'bool', 'indActive needs to be None or a bool'
self.indActive = indActive
@property
def vol(self):
"""
reduced volume vector
:rtype: numpy.array
:return: reduced cell volume
"""
if getattr(self, '_vol', None) is None:
self._vol = self._Pac.T * self.mesh.vol
return self._vol
@property
def nC(self):
"""
reduced number of cells
:rtype: int
:return: number of cells being regularized
"""
if getattr(self, '_nC', None) is None:
if self.indActive is None:
self._nC = self.mesh.nC
else:
self._nC = sum(self.indActive)
return self._nC
@property
def dim(self):
"""
dimension of regularization mesh (1D, 2D, 3D)
:rtype: int
:return: dimension
"""
if getattr(self, '_dim', None) is None:
self._dim = self.mesh.dim
return self._dim
@property
def _Pac(self):
"""
projection matrix that takes from the reduced space of active cells to full modelling space (ie. nC x nindActive)
:rtype: scipy.sparse.csr_matrix
:return: active cell projection matrix
"""
if getattr(self, '__Pac', None) is None:
if self.indActive is None:
self.__Pac = Utils.speye(self.mesh.nC)
else:
self.__Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
return self.__Pac
@property
def _Pafx(self):
"""
projection matrix that takes from the reduced space of active x-faces to full modelling space (ie. nFx x nindActive_Fx )
:rtype: scipy.sparse.csr_matrix
:return: active face-x projection matrix
"""
if getattr(self, '__Pafx', None) is None:
if self.indActive is None:
self.__Pafx = Utils.speye(self.mesh.nFx)
else:
indActive_Fx = (self.mesh.aveFx2CC.T * self.indActive) == 1
self.__Pafx = Utils.speye(self.mesh.nFx)[:,indActive_Fx]
return self.__Pafx
@property
def _Pafy(self):
"""
projection matrix that takes from the reduced space of active y-faces to full modelling space (ie. nFy x nindActive_Fy )
:rtype: scipy.sparse.csr_matrix
:return: active face-y projection matrix
"""
if getattr(self, '__Pafy', None) is None:
if self.indActive is None:
self.__Pafy = Utils.speye(self.mesh.nFy)
else:
indActive_Fy = (self.mesh.aveFy2CC.T * self.indActive) == 1
self.__Pafy = Utils.speye(self.mesh.nFy)[:,indActive_Fy]
return self.__Pafy
@property
def _Pafz(self):
"""
projection matrix that takes from the reduced space of active z-faces to full modelling space (ie. nFz x nindActive_Fz )
:rtype: scipy.sparse.csr_matrix
:return: active face-z projection matrix
"""
if getattr(self, '__Pafz', None) is None:
if self.indActive is None:
self.__Pafz = Utils.speye(self.mesh.nFz)
else:
indActive_Fz = (self.mesh.aveFz2CC.T * self.indActive) == 1
self.__Pafz = Utils.speye(self.mesh.nFz)[:,indActive_Fz]
return self.__Pafz
@property
def aveFx2CC(self):
"""
averaging from active cell centers to active x-faces
:rtype: scipy.sparse.csr_matrix
:return: averaging from active cell centers to active x-faces
"""
if getattr(self, '_aveFx2CC', None) is None:
self._aveFx2CC = self._Pac.T * self.mesh.aveFx2CC * self._Pafx
return self._aveFx2CC
@property
def aveCC2Fx(self):
"""
averaging from active x-faces to active cell centers
:rtype: scipy.sparse.csr_matrix
:return: averaging matrix from active x-faces to active cell centers
"""
if getattr(self, '_aveCC2Fx', None) is None:
self._aveCC2Fx = Utils.sdiag(1./(self.aveFx2CC.T).sum(1)) * self.aveFx2CC.T
return self._aveCC2Fx
@property
def aveFy2CC(self):
"""
averaging from active cell centers to active y-faces
:rtype: scipy.sparse.csr_matrix
:return: averaging from active cell centers to active y-faces
"""
if getattr(self, '_aveFy2CC', None) is None:
self._aveFy2CC = self._Pac.T * self.mesh.aveFy2CC * self._Pafy
return self._aveFy2CC
@property
def aveCC2Fy(self):
"""
averaging from active y-faces to active cell centers
:rtype: scipy.sparse.csr_matrix
:return: averaging matrix from active y-faces to active cell centers
"""
if getattr(self, '_aveCC2Fy', None) is None:
self._aveCC2Fy = Utils.sdiag(1./(self.aveFy2CC.T).sum(1)) * self.aveFy2CC.T
return self._aveCC2Fy
@property
def aveFz2CC(self):
"""
averaging from active cell centers to active z-faces
:rtype: scipy.sparse.csr_matrix
:return: averaging from active cell centers to active z-faces
"""
if getattr(self, '_aveFz2CC', None) is None:
self._aveFz2CC = self._Pac.T * self.mesh.aveFz2CC * self._Pafz
return self._aveFz2CC
@property
def aveCC2Fz(self):
"""
averaging from active z-faces to active cell centers
:rtype: scipy.sparse.csr_matrix
:return: averaging matrix from active z-faces to active cell centers
"""
if getattr(self, '_aveCC2Fz', None) is None:
self._aveCC2Fz = Utils.sdiag(1./(self.aveFz2CC.T).sum(1)) * self.aveFz2CC.T
return self._aveCC2Fz
@property
def cellDiffx(self):
"""
cell centered difference in the x-direction
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active cells in the x-direction
"""
if getattr(self, '_cellDiffx', None) is None:
self._cellDiffx = self._Pafx.T * self.mesh.cellGradx * self._Pac
return self._cellDiffx
@property
def cellDiffy(self):
"""
cell centered difference in the y-direction
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active cells in the y-direction
"""
if getattr(self, '_cellDiffy', None) is None:
self._cellDiffy = self._Pafy.T * self.mesh.cellGrady * self._Pac
return self._cellDiffy
@property
def cellDiffz(self):
"""
cell centered difference in the z-direction
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active cells in the z-direction
"""
if getattr(self, '_cellDiffz', None) is None:
self._cellDiffz = self._Pafz.T * self.mesh.cellGradz * self._Pac
return self._cellDiffz
@property
def faceDiffx(self):
"""
x-face differences
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active faces in the x-direction
"""
if getattr(self, '_faceDiffx', None) is None:
self._faceDiffx = self._Pac.T * self.mesh.faceDivx * self._Pafx
return self._faceDiffx
@property
def faceDiffy(self):
"""
y-face differences
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active faces in the y-direction
"""
if getattr(self, '_faceDiffy', None) is None:
self._faceDiffy = self._Pac.T * self.mesh.faceDivy * self._Pafy
return self._faceDiffy
@property
def faceDiffz(self):
"""
z-face differences
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active faces in the z-direction
"""
if getattr(self, '_faceDiffz', None) is None:
self._faceDiffz = self._Pac.T * self.mesh.faceDivz * self._Pafz
return self._faceDiffz
@property
def cellDiffxStencil(self):
"""
cell centered difference stencil (no cell lengths include) in the x-direction
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active cells in the x-direction
"""
if getattr(self, '_cellDiffxStencil', None) is None:
self._cellDiffxStencil = self._Pafx.T * self.mesh._cellGradxStencil() * self._Pac
return self._cellDiffxStencil
@property
def cellDiffyStencil(self):
"""
cell centered difference stencil (no cell lengths include) in the y-direction
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active cells in the y-direction
"""
if self.dim < 2: return None
if getattr(self, '_cellDiffyStencil', None) is None:
self._cellDiffyStencil = self._Pafy.T * self.mesh._cellGradyStencil() * self._Pac
return self._cellDiffyStencil
@property
def cellDiffzStencil(self):
"""
cell centered difference stencil (no cell lengths include) in the y-direction
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active cells in the y-direction
"""
if self.dim < 3: return None
if getattr(self, '_cellDiffzStencil', None) is None:
self._cellDiffzStencil = self._Pafz.T * self.mesh._cellGradzStencil() * self._Pac
return self._cellDiffzStencil
class BaseRegularization(object):
"""
**Base Regularization Class**
@@ -18,12 +302,19 @@ class BaseRegularization(object):
mapping = None #: A SimPEG.Map instance.
mesh = None #: A SimPEG.Mesh instance.
mref = None #: Reference model.
mref = None #: Reference model.
def __init__(self, mesh, mapping=None, indActive=None, **kwargs):
Utils.setKwargs(self, **kwargs)
self.mesh = mesh
assert isinstance(mesh, Mesh.BaseMesh), "mesh must be a SimPEG.Mesh object."
if indActive is not None and indActive.dtype != 'bool':
tmp = indActive
indActive = np.zeros(mesh.nC, dtype=bool)
indActive[tmp] = True
if indActive is not None and mapping is None:
mapping = Maps.IdentityMap(nP=indActive.nonzero()[0].size)
self.regmesh = RegularizationMesh(mesh,indActive)
self.mapping = mapping or self.mapPair(mesh)
self.mapping._assertMatchesPair(self.mapPair)
self.indActive = indActive
@@ -55,8 +346,7 @@ class BaseRegularization(object):
@property
def W(self):
"""Full regularization weighting matrix W."""
return sp.identity(self.mapping.nP)
return sp.identity(self.regmesh.nC)
@Utils.timeIt
def eval(self, m):
@@ -87,11 +377,12 @@ class BaseRegularization(object):
@Utils.timeIt
def eval2Deriv(self, m, v=None):
"""
Second derivative
:param numpy.array m: geophysical model
:param numpy.array v: vector to multiply
:rtype: scipy.sparse.csr_matrix or numpy.ndarray
:return: WtW or WtW*v
:param numpy.array m: geophysical model
:param numpy.array v: vector to multiply
:rtype: scipy.sparse.csr_matrix or numpy.ndarray
:return: WtW or WtW*v
The regularization is:
@@ -112,112 +403,94 @@ class BaseRegularization(object):
return mD.T * ( self.W.T * ( self.W * ( mD * v) ) )
class Tikhonov(BaseRegularization):
"""
L2 Tikhonov regularization with both smallness and smoothness (first order
derivative) contributions.
.. math::
\phi_m(\mathbf{m}) = \\alpha_s \| W_s (\mathbf{m} - \mathbf{m_{ref}} ) \|^2
+ \\alpha_x \| W_x \\frac{\partial}{\partial x} (\mathbf{m} - \mathbf{m_{ref}} ) \|^2
+ \\alpha_y \| W_y \\frac{\partial}{\partial y} (\mathbf{m} - \mathbf{m_{ref}} ) \|^2
+ \\alpha_z \| W_z \\frac{\partial}{\partial z} (\mathbf{m} - \mathbf{m_{ref}} ) \|^2
Note if the key word argument `mrefInSmooth` is False, then mref is not
included in the smoothness contribution.
:param Mesh mesh: SimPEG mesh
:param Maps mapping: regularization mapping, takes the model from model space to the thing you want to regularize
:param numpy.ndarray indActive: active cell indices for reducing the size of differential operators in the definition of a regularization mesh
:param bool mrefInSmooth: (default = False) put mref in the smoothness component?
:param float alpha_s: (default 1e-6) smallness weight
:param float alpha_x: (default 1) smoothness weight for first derivative in the x-direction
:param float alpha_y: (default 1) smoothness weight for first derivative in the y-direction
:param float alpha_z: (default 1) smoothness weight for first derivative in the z-direction
:param float alpha_xx: (default 1) smoothness weight for second derivative in the x-direction
:param float alpha_yy: (default 1) smoothness weight for second derivative in the y-direction
:param float alpha_zz: (default 1) smoothness weight for second derivative in the z-direction
"""
smoothModel = True #: SMOOTH and SMOOTH_MOD_DIF options
alpha_s = Utils.dependentProperty('_alpha_s', 1e-6, ['_W', '_Ws'], "Smallness weight")
alpha_x = Utils.dependentProperty('_alpha_x', 1.0, ['_W', '_Wx'], "Weight for the first derivative in the x direction")
alpha_y = Utils.dependentProperty('_alpha_y', 1.0, ['_W', '_Wy'], "Weight for the first derivative in the y direction")
alpha_z = Utils.dependentProperty('_alpha_z', 1.0, ['_W', '_Wz'], "Weight for the first derivative in the z direction")
alpha_xx = Utils.dependentProperty('_alpha_xx', 0.0, ['_W', '_Wxx'], "Weight for the second derivative in the x direction")
alpha_yy = Utils.dependentProperty('_alpha_yy', 0.0, ['_W', '_Wyy'], "Weight for the second derivative in the y direction")
alpha_zz = Utils.dependentProperty('_alpha_zz', 0.0, ['_W', '_Wzz'], "Weight for the second derivative in the z direction")
mrefInSmooth = False # put mref in the smoothness contribution
alpha_s = Utils.dependentProperty('_alpha_s', 1e-6, ['_W', '_Wsmall'], "Smallness weight")
alpha_x = Utils.dependentProperty('_alpha_x', 1.0, ['_W', '_Wx'], "Weight for the first derivative in the x direction")
alpha_y = Utils.dependentProperty('_alpha_y', 1.0, ['_W', '_Wy'], "Weight for the first derivative in the y direction")
alpha_z = Utils.dependentProperty('_alpha_z', 1.0, ['_W', '_Wz'], "Weight for the first derivative in the z direction")
alpha_xx = Utils.dependentProperty('_alpha_xx', 0.0, ['_W', '_Wxx'], "Weight for the second derivative in the x direction")
alpha_yy = Utils.dependentProperty('_alpha_yy', 0.0, ['_W', '_Wyy'], "Weight for the second derivative in the y direction")
alpha_zz = Utils.dependentProperty('_alpha_zz', 0.0, ['_W', '_Wzz'], "Weight for the second derivative in the z direction")
def __init__(self, mesh, mapping=None, indActive = None, **kwargs):
BaseRegularization.__init__(self, mesh, mapping=mapping, **kwargs)
self.indActive = indActive
BaseRegularization.__init__(self, mesh, mapping=mapping, indActive=indActive, **kwargs)
@property
def Ws(self):
"""Regularization matrix Ws"""
if getattr(self,'_Ws', None) is None:
self._Ws = Utils.sdiag((self.mesh.vol*self.alpha_s)**0.5)
if self.indActive is not None:
Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
self._Ws = Pac.T * self._Ws * Pac
return self._Ws
def Wsmall(self):
"""Regularization matrix Wsmall"""
if getattr(self,'_Wsmall', None) is None:
self._Wsmall = Utils.sdiag((self.regmesh.vol*self.alpha_s)**0.5)
return self._Wsmall
@property
def Wx(self):
"""Regularization matrix Wx"""
if getattr(self, '_Wx', None) is None:
Ave_x_vol = self.mesh.aveF2CC[:,:self.mesh.nFx].T*self.mesh.vol
self._Wx = Utils.sdiag((Ave_x_vol*self.alpha_x)**0.5)*self.mesh.cellGradx
if self.indActive is not None:
indActive_Fx = (self.mesh.aveFx2CC.T * self.indActive) == 1
Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
Pafx = Utils.speye(self.mesh.nFx)[:,indActive_Fx]
self._Wx = Pafx.T*self._Wx*Pac
Ave_x_vol = self.regmesh.aveCC2Fx * self.regmesh.vol
self._Wx = Utils.sdiag((Ave_x_vol*self.alpha_x)**0.5)*self.regmesh.cellDiffx
return self._Wx
@property
def Wy(self):
"""Regularization matrix Wy"""
if getattr(self, '_Wy', None) is None:
Ave_y_vol = self.mesh.aveF2CC[:,self.mesh.nFx:np.sum(self.mesh.vnF[:2])].T*self.mesh.vol
self._Wy = Utils.sdiag((Ave_y_vol*self.alpha_y)**0.5)*self.mesh.cellGrady
if self.indActive is not None:
indActive_Fy = (self.mesh.aveFy2CC.T * self.indActive) == 1
Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
Pafy = Utils.speye(self.mesh.nFy)[:,indActive_Fy]
self._Wy = Pafy.T*self._Wy*Pac
Ave_y_vol = self.regmesh.aveCC2Fy * self.regmesh.vol
self._Wy = Utils.sdiag((Ave_y_vol*self.alpha_y)**0.5)*self.regmesh.cellDiffy
return self._Wy
@property
def Wz(self):
"""Regularization matrix Wz"""
if getattr(self, '_Wz', None) is None:
Ave_z_vol = self.mesh.aveF2CC[:,np.sum(self.mesh.vnF[:2]):].T*self.mesh.vol
self._Wz = Utils.sdiag((Ave_z_vol*self.alpha_z)**0.5)*self.mesh.cellGradz
if self.indActive is not None:
indActive_Fz = (self.mesh.aveFz2CC.T * self.indActive) == 1
Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
Pafz = Utils.speye(self.mesh.nFz)[:,indActive_Fz]
self._Wz = Pafz.T*self._Wz*Pac
Ave_z_vol = self.regmesh.aveCC2Fz * self.regmesh.vol
self._Wz = Utils.sdiag((Ave_z_vol*self.alpha_z)**0.5)*self.regmesh.cellDiffz
return self._Wz
@property
def Wxx(self):
"""Regularization matrix Wxx"""
if getattr(self, '_Wxx', None) is None:
self._Wxx = Utils.sdiag((self.mesh.vol*self.alpha_xx)**0.5)*self.mesh.faceDivx*self.mesh.cellGradx
if self.indActive is not None:
Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
self._Wxx = Pac.T*self._Wxx*Pac
self._Wxx = Utils.sdiag((self.regmesh.vol*self.alpha_xx)**0.5)*self.regmesh.faceDiffx*self.regmesh.cellDiffx
return self._Wxx
@property
def Wyy(self):
"""Regularization matrix Wyy"""
if getattr(self, '_Wyy', None) is None:
self._Wyy = Utils.sdiag((self.mesh.vol*self.alpha_yy)**0.5)*self.mesh.faceDivy*self.mesh.cellGrady
if self.indActive is not None:
Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
self._Wyy = Pac.T*self._Wyy*Pac
self._Wyy = Utils.sdiag((self.regmesh.vol*self.alpha_yy)**0.5)*self.regmesh.faceDiffy*self.regmesh.cellDiffy
return self._Wyy
@property
def Wzz(self):
"""Regularization matrix Wzz"""
if getattr(self, '_Wzz', None) is None:
self._Wzz = Utils.sdiag((self.mesh.vol*self.alpha_zz)**0.5)*self.mesh.faceDivz*self.mesh.cellGradz
if self.indActive is not None:
Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
self._Wzz = Pac.T*self._Wzz*Pac
self._Wzz = Utils.sdiag((self.regmesh.vol*self.alpha_zz)**0.5)*self.regmesh.faceDiffz*self.regmesh.cellDiffz
return self._Wzz
@property
@@ -225,9 +498,9 @@ class Tikhonov(BaseRegularization):
"""Full smoothness regularization matrix W"""
if getattr(self, '_Wsmooth', None) is None:
wlist = (self.Wx, self.Wxx)
if self.mesh.dim > 1:
if self.regmesh.dim > 1:
wlist += (self.Wy, self.Wyy)
if self.mesh.dim > 2:
if self.regmesh.dim > 2:
wlist += (self.Wz, self.Wzz)
self._Wsmooth = sp.vstack(wlist)
return self._Wsmooth
@@ -236,25 +509,44 @@ class Tikhonov(BaseRegularization):
def W(self):
"""Full regularization matrix W"""
if getattr(self, '_W', None) is None:
wlist = (self.Ws, self.Wsmooth)
wlist = (self.Wsmall, self.Wsmooth)
self._W = sp.vstack(wlist)
return self._W
@Utils.timeIt
def eval(self, m):
if self.smoothModel == True:
r1 = self.Wsmooth * ( self.mapping * (m) )
r2 = self.Ws * ( self.mapping * (m - self.mref) )
return 0.5*(r1.dot(r1)+r2.dot(r2))
elif self.smoothModel == False:
r = self.W * ( self.mapping * (m - self.mref) )
return 0.5*r.dot(r)
def _evalSmall(self, m):
r = self.Wsmall * ( self.mapping * (m - self.mref) )
return 0.5 * r.dot(r)
@Utils.timeIt
def _evalSmooth(self, m):
if self.mrefInSmooth == True:
r = self.Wsmooth * ( self.mapping * (m - self.mref) )
elif self.mrefInSmooth == False:
r = self.Wsmooth * ( self.mapping * (m) )
return 0.5 * r.dot(r)
@Utils.timeIt
def eval(self, m):
return self._evalSmall(m) + self._evalSmooth(m)
@Utils.timeIt
def _evalSmallDeriv(self,m):
r = self.Wsmall * ( self.mapping * (m - self.mref) )
return r.T * ( self.Wsmall * self.mapping.deriv(m - self.mref) )
@Utils.timeIt
def _evalSmoothDeriv(self,m):
if self.mrefInSmooth == True:
r = self.Wsmooth * ( self.mapping * ( m - self.mref ) )
return r.T * ( self.Wsmooth * self.mapping.deriv(m - self.mref) )
elif self.mrefInSmooth == False:
r = self.Wsmooth * ( self.mapping * m )
return r.T * ( self.Wsmooth * self.mapping.deriv(m) )
@Utils.timeIt
def evalDeriv(self, m):
"""
The regularization is:
.. math::
@@ -268,257 +560,185 @@ class Tikhonov(BaseRegularization):
R(m) = \mathbf{W^\\top W (m-m_\\text{ref})}
"""
if self.smoothModel == True:
mD1 = self.mapping.deriv(m)
mD2 = self.mapping.deriv(m - self.mref)
r1 = self.Wsmooth * ( self.mapping * (m))
r2 = self.Ws * ( self.mapping * (m - self.mref) )
out1 = mD1.T * ( self.Wsmooth.T * r1 )
out2 = mD2.T * ( self.Ws.T * r2 )
out = out1+out2
elif self.smoothModel == False:
mD = self.mapping.deriv(m - self.mref)
r = self.W * ( self.mapping * (m - self.mref) )
out = mD.T * ( self.W.T * r )
return out
# <<<<<<< HEAD
# class Simple(BaseRegularization):
# """
# Only for tensor mesh
# """
# smoothModel = True #: SMOOTH and SMOOTH_MOD_DIF options
# alpha_s = Utils.dependentProperty('_alpha_s', 1.0, ['_W', '_Ws'], "Smallness weight")
# alpha_x = Utils.dependentProperty('_alpha_x', 1.0, ['_W', '_Wx'], "Weight for the first derivative in the x direction")
# alpha_y = Utils.dependentProperty('_alpha_y', 1.0, ['_W', '_Wy'], "Weight for the first derivative in the y direction")
# alpha_z = Utils.dependentProperty('_alpha_z', 1.0, ['_W', '_Wz'], "Weight for the first derivative in the z direction")
# alpha_xx = Utils.dependentProperty('_alpha_xx', 0.0, ['_W', '_Wxx'], "Weight for the second derivative in the x direction")
# alpha_yy = Utils.dependentProperty('_alpha_yy', 0.0, ['_W', '_Wyy'], "Weight for the second derivative in the y direction")
# alpha_zz = Utils.dependentProperty('_alpha_zz', 0.0, ['_W', '_Wzz'], "Weight for the second derivative in the z direction")
# def __init__(self, mesh, mapping=None, **kwargs):
# BaseRegularization.__init__(self, mesh, mapping=mapping, **kwargs)
return self._evalSmallDeriv(m) + self._evalSmoothDeriv(m)
class Simple(Tikhonov):
"""
Simple regularization that does not include length scales in the derivatives.
"""
# @property
# def Ws(self):
# """Regularization matrix Ws"""
# if getattr(self,'_Ws', None) is None:
# self._Ws = Utils.sdiag((self.mesh.vol*self.alpha_s)**0.5)
# return self._Ws
mrefInSmooth = False #: SMOOTH and SMOOTH_MOD_DIF options
alpha_s = Utils.dependentProperty('_alpha_s', 1.0, ['_W', '_Wsmall'], "Smallness weight")
alpha_x = Utils.dependentProperty('_alpha_x', 1.0, ['_W', '_Wx'], "Weight for the first derivative in the x direction")
alpha_y = Utils.dependentProperty('_alpha_y', 1.0, ['_W', '_Wy'], "Weight for the first derivative in the y direction")
alpha_z = Utils.dependentProperty('_alpha_z', 1.0, ['_W', '_Wz'], "Weight for the first derivative in the z direction")
wght = 1.
# @property
# def Wx(self):
# """Regularization matrix Wx"""
# if getattr(self, '_Wx', None) is None:
# self._Wx = Utils.sdiag((self.mesh.vol*self.alpha_x)**0.5)*self.mesh.unitCellGradx
# return self._Wx
def __init__(self, mesh, mapping=None, indActive=None, **kwargs):
BaseRegularization.__init__(self, mesh, mapping=mapping, indActive=indActive, **kwargs)
# @property
# def Wy(self):
# """Regularization matrix Wy"""
# if getattr(self, '_Wy', None) is None:
# self._Wy = Utils.sdiag((self.mesh.vol*self.alpha_y)**0.5)*self.mesh.unitCellGrady
# return self._Wy
if isinstance(self.wght,float):
self.wght = np.ones(self.regmesh.nC) * self.wght
# @property
# def Wz(self):
# """Regularization matrix Wz"""
# if getattr(self, '_Wz', None) is None:
# self._Wz = Utils.sdiag((self.mesh.vol*self.alpha_z)**0.5)*self.mesh.unitCellGradz
# return self._Wz
@property
def Wsmall(self):
"""Regularization matrix Wsmall"""
if getattr(self,'_Wsmall', None) is None:
self._Wsmall = Utils.sdiag((self.regmesh.vol*self.alpha_s*self.wght)**0.5)
return self._Wsmall
# @property
# def Wxx(self):
# """Regularization matrix Wxx"""
# if getattr(self, '_Wxx', None) is None:
# self._Wxx = Utils.sdiag((self.mesh.vol*self.alpha_xx)**0.5)*self.mesh.faceDivx*self.mesh.cellGradx
# return self._Wxx
@property
def Wx(self):
"""Regularization matrix Wx"""
if getattr(self, '_Wx', None) is None:
self._Wx = Utils.sdiag((self.regmesh.aveCC2Fx * self.regmesh.vol*self.alpha_x*(self.regmesh.aveCC2Fx*self.wght))**0.5)*self.regmesh.cellDiffxStencil
return self._Wx
# @property
# def Wyy(self):
# """Regularization matrix Wyy"""
# if getattr(self, '_Wyy', None) is None:
# self._Wyy = Utils.sdiag((self.mesh.vol*self.alpha_yy)**0.5)*self.mesh.faceDivy*self.mesh.cellGrady
# return self._Wyy
@property
def Wy(self):
"""Regularization matrix Wy"""
if getattr(self, '_Wy', None) is None:
self._Wy = Utils.sdiag((self.regmesh.aveCC2Fy * self.regmesh.vol * self.alpha_y*(self.regmesh.aveCC2Fy*self.wght))**0.5)*self.regmesh.cellDiffyStencil
return self._Wy
# @property
# def Wzz(self):
# """Regularization matrix Wzz"""
# if getattr(self, '_Wzz', None) is None:
# self._Wzz = Utils.sdiag((self.mesh.vol*self.alpha_zz)**0.5)*self.mesh.faceDivz*self.mesh.cellGradz
# return self._Wzz
@property
def Wz(self):
"""Regularization matrix Wz"""
if getattr(self, '_Wz', None) is None:
self._Wz = Utils.sdiag((self.regmesh.aveCC2Fz * self.regmesh.vol*self.alpha_z*(self.regmesh.aveCC2Fz*self.wght))**0.5)*self.regmesh.cellDiffzStencil
return self._Wz
# @property
# def Wsmooth(self):
# """Full smoothness regularization matrix W"""
# if getattr(self, '_Wsmooth', None) is None:
# wlist = (self.Wx, self.Wxx)
# if self.mesh.dim > 1:
# wlist += (self.Wy, self.Wyy)
# if self.mesh.dim > 2:
# wlist += (self.Wz, self.Wzz)
# self._Wsmooth = sp.vstack(wlist)
# return self._Wsmooth
@property
def Wsmooth(self):
"""Full smoothness regularization matrix W"""
if getattr(self, '_Wsmooth', None) is None:
wlist = (self.Wx,)
if self.regmesh.dim > 1:
wlist += (self.Wy,)
if self.regmesh.dim > 2:
wlist += (self.Wz,)
self._Wsmooth = sp.vstack(wlist)
return self._Wsmooth
# @property
# def W(self):
# """Full regularization matrix W"""
# if getattr(self, '_W', None) is None:
# wlist = (self.Ws, self.Wsmooth)
# self._W = sp.vstack(wlist)
# return self._W
@property
def W(self):
"""Full regularization matrix W"""
if getattr(self, '_W', None) is None:
wlist = (self.Wsmall, self.Wsmooth)
self._W = sp.vstack(wlist)
return self._W
# @Utils.timeIt
# def eval(self, m):
# if self.smoothModel == True:
# r1 = self.Wsmooth * ( self.mapping * (m) )
# r2 = self.Ws * ( self.mapping * (m - self.mref) )
# return 0.5*(r1.dot(r1)+r2.dot(r2))
# elif self.smoothModel == False:
# r = self.W * ( self.mapping * (m - self.mref) )
# return 0.5*r.dot(r)
@Utils.timeIt
def _evalSmall(self, m):
r = self.Wsmall * ( self.mapping * (m - self.mref) )
return 0.5 * r.dot(r)
@Utils.timeIt
def _evalSmooth(self, m):
if self.mrefInSmooth == True:
r = self.Wsmooth * ( self.mapping * (m - self.mref) )
elif self.mrefInSmooth == False:
r = self.Wsmooth * ( self.mapping * m)
return 0.5 * r.dot(r)
# @Utils.timeIt
# def evalDeriv(self, m):
# """
class Sparse(Simple):
# The regularization is:
# set default values
eps_p = 1e-1
eps_q = 1e-1
curModel = None # use a model to compute the weights
gamma = 1.
norms = [0., 2., 2., 2.]
wght = 1.
# .. math::
def __init__(self, mesh, mapping=None, indActive=None, **kwargs):
Simple.__init__(self, mesh, mapping=mapping, indActive=indActive, **kwargs)
# R(m) = \\frac{1}{2}\mathbf{(m-m_\\text{ref})^\\top W^\\top W(m-m_\\text{ref})}
if isinstance(self.wght,float):
self.wght = np.ones(self.regmesh.nC) * self.wght
# So the derivative is straight forward:
@property
def Wsmall(self):
"""Regularization matrix Wsmall"""
if getattr(self, 'curModel', None) is None:
self.Rs = Utils.speye(self.regmesh.nC)
# .. math::
else:
f_m = self.curModel - self.reg.mref
self.rs = self.R(f_m , self.eps_p, self.norms[0])
#print "Min rs: " + str(np.max(self.rs)) + "Max rs: " + str(np.min(self.rs))
self.Rs = Utils.sdiag( self.rs )
# R(m) = \mathbf{W^\\top W (m-m_\\text{ref})}
# """
# if self.smoothModel == True:
# mD1 = self.mapping.deriv(m)
# mD2 = self.mapping.deriv(m - self.mref)
# r1 = self.Wsmooth * ( self.mapping * (m))
# r2 = self.Ws * ( self.mapping * (m - self.mref) )
# out1 = mD1.T * ( self.Wsmooth.T * r1 )
# out2 = mD2.T * ( self.Ws.T * r2 )
# out = out1+out2
# elif self.smoothModel == False:
# mD = self.mapping.deriv(m - self.mref)
# r = self.W * ( self.mapping * (m - self.mref) )
# out = mD.T * ( self.W.T * r )
# return out
# class SparseRegularization(Simple):
# eps = 1e-1
# m = None
# gamma = 1.
# p = 0.
# qx = 2.
# qy = 2.
# qz = 2.
# def __init__(self, mesh, mapping=None, **kwargs):
# Simple.__init__(self, mesh, mapping=mapping, **kwargs)
return Utils.sdiag((self.regmesh.vol*self.alpha_s*self.gamma*self.wght)**0.5)*self.Rs
# @property
# def Wsmooth(self):
# """Full smoothness regularization matrix W"""
# if getattr(self, '_Wsmooth', None) is None:
# wlist = (self.Wx, self.Wxx)
# if self.mesh.dim > 1:
# wlist += (self.Wy, self.Wyy)
# if self.mesh.dim > 2:
# wlist += (self.Wz, self.Wzz)
# self._Wsmooth = sp.vstack(wlist)
# return self._Wsmooth
@property
def Wx(self):
"""Regularization matrix Wx"""
# @property
# def W(self):
# """Full regularization matrix W"""
# if getattr(self, '_W', None) is None:
# wlist = (self.Ws, self.Wsmooth)
# self._W = sp.vstack(wlist)
# return self._W
if getattr(self, 'curModel', None) is None:
self.Rx = Utils.speye(self.regmesh.cellDiffxStencil.shape[0])
# @property
# def Ws(self):
# """Regularization matrix Ws"""
# if getattr(self, 'm', None) is None:
# self.Rs = Utils.speye(self.mesh.nC)
else:
f_m = self.regmesh.cellDiffxStencil * self.curModel
self.rx = self.R( f_m , self.eps_q, self.norms[1])
self.Rx = Utils.sdiag( self.rx )
# else:
# f_m = self.m
# self.rs = self.R(f_m , self.p, self.eps)
# #print "Min rs: " + str(np.max(self.rs)) + "Max rs: " + str(np.min(self.rs))
# self.Rs = Utils.sdiag( self.rs )
return Utils.sdiag(( (self.regmesh.aveCC2Fx * self.regmesh.vol) *self.alpha_x*self.gamma*(self.regmesh.aveCC2Fx*self.wght))**0.5)*self.Rx*self.regmesh.cellDiffxStencil
# self._Ws = Utils.sdiag((self.mesh.vol*self.alpha_s*self.gamma)**0.5)*self.Rs
@property
def Wy(self):
"""Regularization matrix Wy"""
# return self._Ws
if getattr(self, 'curModel', None) is None:
self.Ry = Utils.speye(self.regmesh.cellDiffyStencil.shape[0])
# @property
# def Wx(self):
# """Regularization matrix Wx"""
else:
f_m = self.regmesh.cellDiffyStencil * self.curModel
self.ry = self.R( f_m , self.eps_q, self.norms[2])
self.Ry = Utils.sdiag( self.ry )
# if getattr(self, 'm', None) is None:
# self.Rx = Utils.speye(self.mesh.unitCellGradx.shape[0])
return Utils.sdiag(((self.regmesh.aveCC2Fy * self.regmesh.vol)*self.alpha_y*self.gamma*(self.regmesh.aveCC2Fy*self.wght))**0.5)*self.Ry*self.regmesh.cellDiffyStencil
# else:
# f_m = self.mesh.unitCellGradx * self.m
# self.rx = self.R( f_m , self.qx, self.eps)
# self.Rx = Utils.sdiag( self.rx )
@property
def Wz(self):
"""Regularization matrix Wz"""
# if getattr(self, '_Wx', None) is None:
# self._Wx = Utils.sdiag((self.mesh.vol*self.alpha_x*self.gamma)**0.5)*self.Rx*self.mesh.unitCellGradx
# return self._Wx
if getattr(self, 'curModel', None) is None:
self.Rz = Utils.speye(self.regmesh.cellDiffzStencil.shape[0])
# @property
# def Wy(self):
# """Regularization matrix Wy"""
else:
f_m = self.regmesh.cellDiffzStencil * self.curModel
self.rz = self.R( f_m , self.eps_q, self.norms[3])
self.Rz = Utils.sdiag( self.rz )
# if getattr(self, 'm', None) is None:
# self.Ry = Utils.speye(self.mesh.unitCellGrady.shape[0])
return Utils.sdiag(((self.regmesh.aveCC2Fz * self.regmesh.vol)*self.alpha_z*self.gamma*(self.regmesh.aveCC2Fz*self.wght))**0.5)*self.Rz*self.regmesh.cellDiffzStencil
# else:
# f_m = self.mesh.unitCellGrady * self.m
# self.ry = self.R( f_m , self.qy, self.eps)
# self.Ry = Utils.sdiag( self.ry )
@property
def Wsmooth(self):
"""Full smoothness regularization matrix W"""
#if getattr(self, '_Wsmooth', None) is None:
wlist = (self.Wx,)
if self.regmesh.dim > 1:
wlist += (self.Wy,)
if self.regmesh.dim > 2:
wlist += (self.Wz,)
#self._Wsmooth = sp.vstack(wlist)
return sp.vstack(wlist)
# if getattr(self, '_Wy', None) is None:
# self._Wy = Utils.sdiag((self.mesh.vol*self.alpha_y*self.gamma)**0.5)*self.Ry*self.mesh.unitCellGrady
# return self._Wy
@property
def W(self):
"""Full regularization matrix W"""
if getattr(self, '_W', None) is None:
wlist = (self.Wsmall, self.Wsmooth)
self._W = sp.vstack(wlist)
return self._W
# @property
# def Wz(self):
# """Regularization matrix Wz"""
def R(self, f_m , eps, exponent):
# if getattr(self, 'm', None) is None:
# self.Rz = Utils.speye(self.mesh.unitCellGradz.shape[0])
eta = (eps**(1.-exponent/2.))**0.5
r = eta / (f_m**2.+ eps**2.)**((1.-exponent/2.)/2.)
# else:
# f_m = self.mesh.unitCellGradz * self.m
# self.rz = self.R( f_m , self.qz, self.eps)
# self.Rz = Utils.sdiag( self.rz )
# if getattr(self, '_Wz', None) is None:
# self._Wz = Utils.sdiag((self.mesh.vol*self.alpha_z*self.gamma)**0.5)*self.Rz*self.mesh.unitCellGradz
# return self._Wz
# def R(self, f_m , p, dec):
# eta = (self.eps**(1-p/2.))**0.5
# r = eta / (f_m**2.+self.eps**2.)**((1-p/2.)/2.)
# return r
# =======
# >>>>>>> 834de582844e8e1eac95819fbe03eed55dbeb001
return r
+14 -4
View File
@@ -88,12 +88,14 @@ def getIndicesBlock(p0,p1,ccMesh):
# Return a tuple
return ind
def defineBlock(ccMesh,p0,p1,vals=[0,1]):
def defineBlock(ccMesh,p0,p1,vals=None):
"""
Build a block with the conductivity specified by condVal. Returns an array.
vals[0] conductivity of the block
vals[1] conductivity of the ground
"""
if vals is None:
vals = [0,1]
sigma = np.zeros(ccMesh.shape[0]) + vals[1]
ind = getIndicesBlock(p0,p1,ccMesh)
@@ -101,7 +103,11 @@ def defineBlock(ccMesh,p0,p1,vals=[0,1]):
return mkvc(sigma)
def defineElipse(ccMesh, center=[0,0,0], anisotropy=[1,1,1], slope=10., theta=0.):
def defineElipse(ccMesh, center=None, anisotropy=None, slope=10., theta=0.):
if center is None:
center = [0,0,0]
if anisotropy is None:
anisotropy = [1,1,1]
G = ccMesh.copy()
dim = ccMesh.shape[1]
for i in range(dim):
@@ -156,7 +162,7 @@ def getIndicesSphere(center,radius,ccMesh):
# Return a tuple
return ind
def defineTwoLayers(ccMesh,depth,vals=[0,1]):
def defineTwoLayers(ccMesh,depth,vals=None):
"""
Define a two layered model. Depth of the first layer must be specified.
CondVals vector with the conductivity values of the layers. Eg:
@@ -167,6 +173,8 @@ def defineTwoLayers(ccMesh,depth,vals=[0,1]):
0 depth zf
1st layer 2nd layer
"""
if vals is None:
vals = [0,1]
sigma = np.zeros(ccMesh.shape[0]) + vals[1]
dim = np.size(ccMesh[0,:])
@@ -252,7 +260,7 @@ def layeredModel(ccMesh, layerTops, layerValues):
def randomModel(shape, seed=None, anisotropy=None, its=100, bounds=[0,1]):
def randomModel(shape, seed=None, anisotropy=None, its=100, bounds=None):
"""
Create a random model by convolving a kernel with a
uniformly distributed model.
@@ -276,6 +284,8 @@ def randomModel(shape, seed=None, anisotropy=None, its=100, bounds=[0,1]):
"""
if bounds is None:
bounds = [0,1]
if seed is None:
seed = np.random.randint(1e3)
+3 -1
View File
@@ -55,8 +55,10 @@ def hook(obj, method, name=None, overwrite=False, silent=False):
print 'Method '+name+' was not overwritten.'
def setKwargs(obj, ignore=[], **kwargs):
def setKwargs(obj, ignore=None, **kwargs):
"""Sets key word arguments (kwargs) that are present in the object, throw an error if they don't exist."""
if ignore is None:
ignore = []
for attr in kwargs:
if attr in ignore:
continue
+137
View File
@@ -0,0 +1,137 @@
from SimPEG import np, Mesh
import time as tm
import vtk, vtk.util.numpy_support as npsup
import re
def read_GOCAD_ts(tsfile):
"""
Read GOCAD triangulated surface (*.ts) file
INPUT:
tsfile: Triangulated surface
OUTPUT:
vrts : Array of vertices in XYZ coordinates [n x 3]
trgl : Array of index for triangles [m x 3]. The order of the vertices
is important and describes the normal
n = cross( (P2 - P1 ) , (P3 - P1) )
Author: @fourndo
.. note::
Remove all attributes from the GoCAD surface before exporting it!
"""
fid = open(tsfile,'r')
line = fid.readline()
# Skip all the lines until the vertices
while re.match('TFACE',line)==None:
line = fid.readline()
line = fid.readline()
vrtx = []
# Run down all the vertices and save in array
while re.match('VRTX',line):
l_input = re.split('[\s*]',line)
temp = np.array(l_input[2:5])
vrtx.append(temp.astype(np.float))
# Read next line
line = fid.readline()
vrtx = np.asarray(vrtx)
# Skip lines to the triangles
while re.match('TRGL',line)==None:
line = fid.readline()
# Run down the list of triangles
trgl = []
# Run down all the vertices and save in array
while re.match('TRGL',line):
l_input = re.split('[\s*]',line)
temp = np.array(l_input[1:4])
trgl.append(temp.astype(np.int))
# Read next line
line = fid.readline()
trgl = np.asarray(trgl)
return vrtx, trgl
def surface2inds(vrtx, trgl, mesh, boundaries=True, internal=True):
""""
Function to read gocad polystructure file and output indexes of mesh with in the structure.
"""
# Adjust the index
trgl = trgl - 1
# Make vtk pts
ptsvtk = vtk.vtkPoints()
ptsvtk.SetData(npsup.numpy_to_vtk(vrtx,deep=1))
# Make the polygon connection
polys = vtk.vtkCellArray()
for face in trgl:
poly = vtk.vtkPolygon()
poly.GetPointIds().SetNumberOfIds(len(face))
for nrv, vert in enumerate(face):
poly.GetPointIds().SetId(nrv,vert)
polys.InsertNextCell(poly)
# Make the polydata, structure of connections and vrtx
polyData = vtk.vtkPolyData()
polyData.SetPoints(ptsvtk)
polyData.SetPolys(polys)
# Make implicit func
ImpDistFunc = vtk.vtkImplicitPolyDataDistance()
ImpDistFunc.SetInput(polyData)
# Convert the mesh
vtkMesh = vtk.vtkRectilinearGrid()
vtkMesh.SetDimensions(mesh.nNx,mesh.nNy,mesh.nNz)
vtkMesh.SetXCoordinates(npsup.numpy_to_vtk(mesh.vectorNx, deep=1))
vtkMesh.SetYCoordinates(npsup.numpy_to_vtk(mesh.vectorNy, deep=1))
vtkMesh.SetZCoordinates(npsup.numpy_to_vtk(mesh.vectorNz, deep=1))
# Add indexes
vtkInd = npsup.numpy_to_vtk(np.arange(mesh.nC), deep=1)
vtkInd.SetName('Index')
vtkMesh.GetCellData().AddArray(vtkInd)
extractImpDistRectGridFilt = vtk.vtkExtractGeometry() # Object constructor
extractImpDistRectGridFilt.SetImplicitFunction(ImpDistFunc) #
extractImpDistRectGridFilt.SetInputData(vtkMesh)
if boundaries is True:
extractImpDistRectGridFilt.ExtractBoundaryCellsOn()
else:
extractImpDistRectGridFilt.ExtractBoundaryCellsOff()
if internal is True:
extractImpDistRectGridFilt.ExtractInsideOn()
else:
extractImpDistRectGridFilt.ExtractInsideOff()
print "Extracting indices from grid..."
# Executing the pipe
extractImpDistRectGridFilt.Update()
# Get index inside
insideGrid = extractImpDistRectGridFilt.GetOutput()
insideGrid = npsup.vtk_to_numpy(insideGrid.GetCellData().GetArray('Index'))
# Return the indexes inside
return insideGrid
+9 -1
View File
@@ -12,8 +12,16 @@
DC Forward Simulation
=====================
Forward model conductive spheres in a half-space and plot a pseudo-section
Forward model two conductive spheres in a half-space and plot a
pseudo-section. Assumes an infinite line source and measures along the
center of the spheres.
INPUT:
loc = Location of spheres [[x1,y1,z1],[x2,y2,z2]]
radi = Radius of spheres [r1,r2]
param = Conductivity of background and two spheres [m0,m1,m2]
stype = survey type "pdp" (pole dipole) or "dpdp" (dipole dipole)
dtype = Data type "appr" (app res) | "appc" (app cond) | "volt" (potential)
Created by @fourndo on Mon Feb 01 19:28:06 2016
@@ -0,0 +1,58 @@
.. _examples_EM_Schenkel_Morrison_Casing:
.. --------------------------------- ..
.. ..
.. THIS FILE IS AUTO GENEREATED ..
.. ..
.. SimPEG/Examples/__init__.py ..
.. ..
.. --------------------------------- ..
EM: Schenkel and Morrison Casing Model
======================================
Here we create and run a FDEM forward simulation to calculate the vertical
current inside a steel-cased. The model is based on the Schenkel and
Morrison Casing Model, and the results are used in a 2016 SEG abstract by
Yang et al.
- Schenkel, C.J., and H.F. Morrison, 1990, Effects of well casing on potential field measurements using downhole current sources: Geophysical prospecting, 38, 663-686.
The model consists of:
- Air: Conductivity 1e-8 S/m, above z = 0
- Background: conductivity 1e-2 S/m, below z = 0
- Casing: conductivity 1e6 S/m
- 300m long
- radius of 0.1m
- thickness of 6e-3m
Inside the casing, we take the same conductivity as the background.
We are using an EM code to simulate DC, so we use frequency low enough
that the skin depth inside the casing is longer than the casing length (f
= 1e-6 Hz). The plot produced is of the current inside the casing.
These results are shown in the SEG abstract by Yang et al., 2016: 3D DC
resistivity modeling of steel casing for reservoir monitoring using
equivalent resistor network. The solver used to produce these results and
achieve the CPU time of ~30s is Mumps, which was installed using pymatsolver_
.. _pymatsolver: https://github.com/rowanc1/pymatsolver
This example is on figshare: https://dx.doi.org/10.6084/m9.figshare.3126961.v1
If you would use this example for a code comparison, or build upon it, a
citation would be much appreciated!
.. plot::
from SimPEG import Examples
Examples.EM_Schenkel_Morrison_Casing.run()
.. literalinclude:: ../../SimPEG/Examples/EM_Schenkel_Morrison_Casing.py
:language: python
:linenos:
+26
View File
@@ -0,0 +1,26 @@
.. _examples_Inversion_IRLS:
.. --------------------------------- ..
.. ..
.. THIS FILE IS AUTO GENEREATED ..
.. ..
.. SimPEG/Examples/__init__.py ..
.. ..
.. --------------------------------- ..
Inversion: Linear Problem
=========================
Here we go over the basics of creating a linear problem and inversion.
.. plot::
from SimPEG import Examples
Examples.Inversion_IRLS.run()
.. literalinclude:: ../../SimPEG/Examples/Inversion_IRLS.py
:language: python
:linenos:
+73 -49
View File
@@ -5,6 +5,8 @@ from scipy.sparse.linalg import dsolve
import inspect
TOL = 1e-20
testReg = True
testRegMesh = True
class RegularizationTests(unittest.TestCase):
@@ -16,44 +18,80 @@ class RegularizationTests(unittest.TestCase):
mesh3 = Mesh.TensorMesh([hx, hy, hz])
self.meshlist = [mesh1,mesh2, mesh3]
def test_regularization(self):
for R in dir(Regularization):
r = getattr(Regularization, R)
if not inspect.isclass(r): continue
if not issubclass(r, Regularization.BaseRegularization):
continue
if testReg:
def test_regularization(self):
for R in dir(Regularization):
r = getattr(Regularization, R)
if not inspect.isclass(r): continue
if not issubclass(r, Regularization.BaseRegularization):
continue
for i, mesh in enumerate(self.meshlist):
print 'Testing %iD'%mesh.dim
mapping = r.mapPair(mesh)
reg = r(mesh, mapping=mapping)
m = np.random.rand(mapping.nP)
reg.mref = np.ones_like(m)*np.mean(m)
print 'Check: phi_m (mref) = %f' %reg.eval(reg.mref)
passed = reg.eval(reg.mref) < TOL
self.assertTrue(passed)
print 'Check:', R
passed = Tests.checkDerivative(lambda m : [reg.eval(m), reg.evalDeriv(m)], m, plotIt=False)
self.assertTrue(passed)
print 'Check 2 Deriv:', R
passed = Tests.checkDerivative(lambda m : [reg.evalDeriv(m), reg.eval2Deriv(m)], m, plotIt=False)
self.assertTrue(passed)
def test_regularization_ActiveCells(self):
for R in dir(Regularization):
r = getattr(Regularization, R)
if not inspect.isclass(r): continue
if not issubclass(r, Regularization.BaseRegularization):
continue
for i, mesh in enumerate(self.meshlist):
print 'Testing Active Cells %iD'%(mesh.dim)
if mesh.dim == 1:
indActive = Utils.mkvc(mesh.gridCC <= 0.8)
elif mesh.dim == 2:
indActive = Utils.mkvc(mesh.gridCC[:,-1] <= 2*np.sin(2*np.pi*mesh.gridCC[:,0])+0.5)
elif mesh.dim == 3:
indActive = Utils.mkvc(mesh.gridCC[:,-1] <= 2*np.sin(2*np.pi*mesh.gridCC[:,0])+0.5 * 2*np.sin(2*np.pi*mesh.gridCC[:,1])+0.5)
for indAct in [indActive, indActive.nonzero()[0]]: # test both bool and integers
reg = r(mesh, indActive=indAct)
m = np.random.rand(mesh.nC)[indAct]
reg.mref = np.ones_like(m)*np.mean(m)
print 'Check: phi_m (mref) = %f' %reg.eval(reg.mref)
passed = reg.eval(reg.mref) < TOL
self.assertTrue(passed)
print 'Check:', R
passed = Tests.checkDerivative(lambda m : [reg.eval(m), reg.evalDeriv(m)], m, plotIt=False)
self.assertTrue(passed)
print 'Check 2 Deriv:', R
passed = Tests.checkDerivative(lambda m : [reg.evalDeriv(m), reg.eval2Deriv(m)], m, plotIt=False)
self.assertTrue(passed)
if testRegMesh:
def test_regularizationMesh(self):
for i, mesh in enumerate(self.meshlist):
print 'Testing %iD'%mesh.dim
mapping = r.mapPair(mesh)
reg = r(mesh, mapping=mapping)
m = np.random.rand(mapping.nP)
reg.mref = np.ones_like(m)*np.mean(m)
print 'Check: phi_m (mref) = %f' %reg.eval(reg.mref)
passed = reg.eval(reg.mref) < TOL
self.assertTrue(passed)
print 'Check:', R
passed = Tests.checkDerivative(lambda m : [reg.eval(m), reg.evalDeriv(m)], m, plotIt=False)
self.assertTrue(passed)
print 'Check 2 Deriv:', R
passed = Tests.checkDerivative(lambda m : [reg.evalDeriv(m), reg.eval2Deriv(m)], m, plotIt=False)
self.assertTrue(passed)
def test_regularization_ActiveCells(self):
for R in dir(Regularization):
r = getattr(Regularization, R)
if not inspect.isclass(r): continue
if not issubclass(r, Regularization.BaseRegularization):
continue
for i, mesh in enumerate(self.meshlist):
print 'Testing Active Cells %iD'%(mesh.dim)
# mapping = r.mapPair(mesh)
# reg = r(mesh, mapping=mapping)
# m = np.random.rand(mapping.nP)
if mesh.dim == 1:
indAct = Utils.mkvc(mesh.gridCC <= 0.8)
@@ -62,23 +100,9 @@ class RegularizationTests(unittest.TestCase):
elif mesh.dim == 3:
indAct = Utils.mkvc(mesh.gridCC[:,-1] <= 2*np.sin(2*np.pi*mesh.gridCC[:,0])+0.5 * 2*np.sin(2*np.pi*mesh.gridCC[:,1])+0.5)
mapping = Maps.IdentityMap(nP=indAct.nonzero()[0].size)
regmesh = Regularization.RegularizationMesh(mesh, indActive=indAct)
reg = r(mesh, mapping=mapping, indActive=indAct)
m = np.random.rand(mesh.nC)[indAct]
reg.mref = np.ones_like(m)*np.mean(m)
print 'Check: phi_m (mref) = %f' %reg.eval(reg.mref)
passed = reg.eval(reg.mref) < TOL
self.assertTrue(passed)
print 'Check:', R
passed = Tests.checkDerivative(lambda m : [reg.eval(m), reg.evalDeriv(m)], m, plotIt=False)
self.assertTrue(passed)
print 'Check 2 Deriv:', R
passed = Tests.checkDerivative(lambda m : [reg.evalDeriv(m), reg.eval2Deriv(m)], m, plotIt=False)
self.assertTrue(passed)
assert (regmesh.vol == mesh.vol[indAct]).all()
if __name__ == '__main__':
+3 -1
View File
@@ -10,7 +10,9 @@ except ImportError, e:
MumpsSolver = SolverLU
def halfSpaceProblemAnaDiff(meshType, sig_half=1e-2, rxOffset=50., bounds=[1e-5,1e-3], showIt=False):
def halfSpaceProblemAnaDiff(meshType, sig_half=1e-2, rxOffset=50., bounds=None, showIt=False):
if bounds is None:
bounds = [1e-5,1e-3]
if meshType == 'CYL':
cs, ncx, ncz, npad = 5., 30, 10, 15
hx = [(cs,ncx), (cs,npad,1.3)]
+80 -4
View File
@@ -146,6 +146,20 @@ class TestCyl2DMesh(unittest.TestCase):
assert np.abs(Pr*(Pc2r*mc) - Pc*mc).max() < 1e-3
def test_getInterpMatCartMesh_Cells2Nodes(self):
Mr = Mesh.TensorMesh([100,100,2], x0='CC0')
Mc = Mesh.CylMesh([np.ones(10)/5,1,10],x0='0C0',cartesianOrigin=[-0.2,-0.2,0])
mc = np.arange(Mc.nC)
xr = np.linspace(0,0.4,50)
xc = np.linspace(0,0.4,50) + 0.2
Pr = Mr.getInterpolationMat(np.c_[xr,np.ones(50)*-0.2,np.ones(50)*0.5],'N')
Pc = Mc.getInterpolationMat(np.c_[xc,np.zeros(50),np.ones(50)*0.5],'CC')
Pc2r = Mc.getInterpolationMatCartMesh(Mr, 'CC', locTypeTo='N')
assert np.abs(Pr*(Pc2r*mc) - Pc*mc).max() < 1e-3
def test_getInterpMatCartMesh_Faces(self):
Mr = Mesh.TensorMesh([100,100,2], x0='CC0')
@@ -177,6 +191,37 @@ class TestCyl2DMesh(unittest.TestCase):
assert np.abs(mag[dist > 0.1].min() - 1) < TOL
def test_getInterpMatCartMesh_Faces2Edges(self):
Mr = Mesh.TensorMesh([100,100,2], x0='CC0')
Mc = Mesh.CylMesh([np.ones(10)/5,1,10],x0='0C0',cartesianOrigin=[-0.2,-0.2,0])
Pf2e = Mc.getInterpolationMatCartMesh(Mr, 'F', locTypeTo='E')
mf = np.ones(Mc.nF)
ecart = Pf2e * mf
excc = Mr.aveEx2CC*Mr.r(ecart, 'E', 'Ex')
eycc = Mr.aveEy2CC*Mr.r(ecart, 'E', 'Ey')
ezcc = Mr.r(ecart, 'E', 'Ez')
indX = Utils.closestPoints(Mr, [0.45, -0.2, 0.5])
indY = Utils.closestPoints(Mr, [-0.2, 0.45, 0.5])
TOL = 1e-2
assert np.abs(float(excc[indX]) - 1) < TOL
assert np.abs(float(excc[indY]) - 0) < TOL
assert np.abs(float(eycc[indX]) - 0) < TOL
assert np.abs(float(eycc[indY]) - 1) < TOL
assert np.abs((ezcc - 1).sum()) < TOL
mag = (excc**2 + eycc**2)**0.5
dist = ((Mr.gridCC[:,0] + 0.2)**2 + (Mr.gridCC[:,1] + 0.2)**2)**0.5
assert np.abs(mag[dist > 0.1].max() - 1) < TOL
assert np.abs(mag[dist > 0.1].min() - 1) < TOL
def test_getInterpMatCartMesh_Edges(self):
Mr = Mesh.TensorMesh([100,100,2], x0='CC0')
@@ -185,11 +230,42 @@ class TestCyl2DMesh(unittest.TestCase):
Pe = Mc.getInterpolationMatCartMesh(Mr, 'E')
me = np.ones(Mc.nE)
erect = Pe * me
ecart = Pe * me
excc = Mr.aveEx2CC*Mr.r(erect, 'E', 'Ex')
eycc = Mr.aveEy2CC*Mr.r(erect, 'E', 'Ey')
ezcc = Mr.r(erect, 'E', 'Ez')
excc = Mr.aveEx2CC*Mr.r(ecart, 'E', 'Ex')
eycc = Mr.aveEy2CC*Mr.r(ecart, 'E', 'Ey')
ezcc = Mr.aveEz2CC*Mr.r(ecart, 'E', 'Ez')
indX = Utils.closestPoints(Mr, [0.45, -0.2, 0.5])
indY = Utils.closestPoints(Mr, [-0.2, 0.45, 0.5])
TOL = 1e-2
assert np.abs(float(excc[indX]) - 0) < TOL
assert np.abs(float(excc[indY]) + 1) < TOL
assert np.abs(float(eycc[indX]) - 1) < TOL
assert np.abs(float(eycc[indY]) - 0) < TOL
assert np.abs(ezcc.sum()) < TOL
mag = (excc**2 + eycc**2)**0.5
dist = ((Mr.gridCC[:,0] + 0.2)**2 + (Mr.gridCC[:,1] + 0.2)**2)**0.5
assert np.abs(mag[dist > 0.1].max() - 1) < TOL
assert np.abs(mag[dist > 0.1].min() - 1) < TOL
def test_getInterpMatCartMesh_Edges2Faces(self):
Mr = Mesh.TensorMesh([100,100,2], x0='CC0')
Mc = Mesh.CylMesh([np.ones(10)/5,1,10],x0='0C0',cartesianOrigin=[-0.2,-0.2,0])
Pe2f = Mc.getInterpolationMatCartMesh(Mr, 'E', locTypeTo='F')
me = np.ones(Mc.nE)
frect = Pe2f * me
excc = Mr.aveFx2CC*Mr.r(frect, 'F', 'Fx')
eycc = Mr.aveFy2CC*Mr.r(frect, 'F', 'Fy')
ezcc = Mr.r(frect, 'F', 'Fz')
indX = Utils.closestPoints(Mr, [0.45, -0.2, 0.5])
indY = Utils.closestPoints(Mr, [-0.2, 0.45, 0.5])
@@ -242,9 +242,6 @@ class TestAnalytics(unittest.TestCase):
def test_appRes1en3(self):self.assertTrue(appResPhsHalfspace_eFrom_ps_Norm(1e-3))
def test_appPhs1en3(self):self.assertTrue(appResPhsHalfspace_eFrom_ps_Norm(1e-3,False))
# Do a derivative test
def test_derivProj1(self):self.assertTrue(DerivProjfieldsTest(halfSpace(1e-2)))
# Do a derivative test of Jvec
# def test_derivJvec_zxxr(self):self.assertTrue(DerivJvecTest(random(1e-2),'zxxr',.1))
# def test_derivJvec_zxxi(self):self.assertTrue(DerivJvecTest(random(1e-2),'zxxi',.1))